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Solution Manual For Calculus Single Variable, 8th Edition by Deborah Hughes-Hallett, Andrew M. Gleas

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1.1 SOLUTIONS

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CHAPTER ONE Solutions for Section 1.1 EXERCISES 1. Since 𝑑 represents the number of years since 2020, we see that 𝑓 (5) represents the population of the city in 2025. In 2025, the city’s population is 8 million. 2. Since 𝑇 = 𝑓 (𝑃 ), we see that 𝑓 (200) is the value of 𝑇 when 𝑃 = 200; that is, the thickness of pelican eggs when the concentration of PCBs is 200 ppm. 3. If there are no workers, there is no productivity, so the graph goes through the origin. At first, as the number of workers increases, productivity also increases. As a result, the curve goes up initially. At a certain point the curve reaches its highest level, after which it goes downward; in other words, as the number of workers increases beyond that point, productivity decreases. This might, for example, be due either to the inefficiency inherent in large organizations or simply to workers getting in each other’s way as too many are crammed on the same line. Many other reasons are possible. 4. (a) is (V), because slope is positive, vertical intercept is negative (b) is (IV), because slope is negative, vertical intercept is positive (c) is (I), because slope is 0, vertical intercept is positive (d) is (VI), because slope and vertical intercept are both negative (e) is (II), because slope and vertical intercept are both positive (f) is (III), because slope is positive, vertical intercept is 0 5. (a) is (V), because slope is negative, vertical intercept is 0 (b) is (VI), because slope and vertical intercept are both positive (c) is (I), because slope is negative, vertical intercept is positive (d) is (IV), because slope is positive, vertical intercept is negative (e) is (III), because slope and vertical intercept are both negative (f) is (II), because slope is positive, vertical intercept is 0 6. The slope is (1 βˆ’ 0)βˆ•(1 βˆ’ 0) = 1. So the equation of the line is 𝑦 = π‘₯. 7. The slope is (3 βˆ’ 2)βˆ•(2 βˆ’ 0) = 1βˆ•2. So the equation of the line is 𝑦 = (1βˆ•2)π‘₯ + 2. 8. The slope is

2 1 3βˆ’1 = = . 2 βˆ’ (βˆ’2) 4 2 Now we know that 𝑦 = (1βˆ•2)π‘₯ + 𝑏. Using the point (βˆ’2, 1), we have 1 = βˆ’2βˆ•2 + 𝑏, which yields 𝑏 = 2. Thus, the equation of the line is 𝑦 = (1βˆ•2)π‘₯ + 2. 6βˆ’0 9. The slope is = 2 so the equation of the line is 𝑦 βˆ’ 6 = 2(π‘₯ βˆ’ 2) or 𝑦 = 2π‘₯ + 2. 2 βˆ’ (βˆ’1) 5 5 10. Rewriting the equation as 𝑦 = βˆ’ π‘₯ + 4 shows that the slope is βˆ’ and the vertical intercept is 4. 2 2 11. Rewriting the equation as 2 12 𝑦=βˆ’ π‘₯+ 7 7 shows that the line has slope βˆ’12βˆ•7 and vertical intercept 2βˆ•7. Slope =

12. Rewriting the equation of the line as βˆ’2 π‘₯βˆ’2 4 1 𝑦 = π‘₯ + 2, 2

βˆ’π‘¦ =

we see the line has slope 1βˆ•2 and vertical intercept 2.


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Chapter One /SOLUTIONS 13. Rewriting the equation of the line as 12 4 π‘₯βˆ’ 6 6 2 𝑦 = 2π‘₯ βˆ’ , 3 𝑦=

we see that the line has slope 2 and vertical intercept βˆ’2βˆ•3. 14. The intercepts appear to be (0, 3) and (7.5, 0), giving Slope =

6 2 βˆ’3 =βˆ’ =βˆ’ . 7.5 15 5

The 𝑦-intercept is at (0, 3), so a possible equation for the line is 2 𝑦 = βˆ’ π‘₯ + 3. 5 (Answers may vary.) 15. 𝑦 βˆ’ 𝑐 = π‘š(π‘₯ βˆ’ π‘Ž) 16. Given that the function is linear, choose any two points, for example (5.2, 27.8) and (5.3, 29.2). Then Slope =

29.2 βˆ’ 27.8 1.4 = = 14. 5.3 βˆ’ 5.2 0.1

Using the point-slope formula, with the point (5.2, 27.8), we get the equation 𝑦 βˆ’ 27.8 = 14(π‘₯ βˆ’ 5.2) which is equivalent to 𝑦 = 14π‘₯ βˆ’ 45. 17. 𝑦 = 5π‘₯ βˆ’ 3. Since the slope of this line is 5, we want a line with slope βˆ’ 15 passing through the point (2, 1). The equation is (𝑦 βˆ’ 1) = βˆ’ 15 (π‘₯ βˆ’ 2), or 𝑦 = βˆ’ 15 π‘₯ + 75 .

18. The line 𝑦 + 4π‘₯ = 7 has slope βˆ’4. Therefore the parallel line has slope βˆ’4 and equation 𝑦 βˆ’ 5 = βˆ’4(π‘₯ βˆ’ 1) or 𝑦 = βˆ’4π‘₯ + 9. βˆ’1 = 14 and equation 𝑦 βˆ’ 5 = 14 (π‘₯ βˆ’ 1) or 𝑦 = 0.25π‘₯ + 4.75. The perpendicular line has slope (βˆ’4) 19. The line parallel to 𝑦 = π‘šπ‘₯ + 𝑐 also has slope π‘š, so its equation is 𝑦 = π‘š(π‘₯ βˆ’ π‘Ž) + 𝑏. The line perpendicular to 𝑦 = π‘šπ‘₯ + 𝑐 has slope βˆ’1βˆ•π‘š, so its equation will be 1 𝑦 = βˆ’ (π‘₯ βˆ’ π‘Ž) + 𝑏. π‘š 20. Since the function goes from π‘₯ = 0 to π‘₯ = 4 and between 𝑦 = 0 and 𝑦 = 2, the domain is 0 ≀ π‘₯ ≀ 4 and the range is 0 ≀ 𝑦 ≀ 2. 21. Since π‘₯ goes from 1 to 5 and 𝑦 goes from 1 to 6, the domain is 1 ≀ π‘₯ ≀ 5 and the range is 1 ≀ 𝑦 ≀ 6. 22. Since the function goes from π‘₯ = βˆ’2 to π‘₯ = 2 and from 𝑦 = βˆ’2 to 𝑦 = 2, the domain is βˆ’2 ≀ π‘₯ ≀ 2 and the range is βˆ’2 ≀ 𝑦 ≀ 2. 23. Since the function goes from π‘₯ = 0 to π‘₯ = 5 and between 𝑦 = 0 and 𝑦 = 4, the domain is 0 ≀ π‘₯ ≀ 5 and the range is 0 ≀ 𝑦 ≀ 4. 24. The domain is all numbers. The range is all numbers β‰₯ 2, since π‘₯2 β‰₯ 0 for all π‘₯. 25. The domain is all π‘₯-values, as the denominator is never zero. The range is 0 < 𝑦 ≀

1 . 2


1.1 SOLUTIONS

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26. The value of 𝑓 (𝑑) is real provided 𝑑2 βˆ’ 16 β‰₯ 0 or 𝑑2 β‰₯ 16. This occurs when either 𝑑 β‰₯ 4, or 𝑑 ≀ βˆ’4. Solving 𝑓 (𝑑) = 3, we have √ 𝑑2 βˆ’ 16 = 3 𝑑2 βˆ’ 16 = 9 𝑑2 = 25 so 𝑑 = Β±5. 27. We have 𝑉 = π‘˜π‘Ÿ3 . You may know that 𝑉 = 𝑑 . 𝑑 29. For some constant π‘˜, we have 𝑆 = π‘˜β„Ž2 .

4 3 πœ‹π‘Ÿ . 3

28. If distance is 𝑑, then 𝑣 =

30. We know that 𝐸 is proportional to 𝑣3 , so 𝐸 = π‘˜π‘£3 , for some constant π‘˜. 31. We know that 𝑁 is proportional to 1βˆ•π‘™2 , so 𝑁=

π‘˜ , 𝑙2

for some constant π‘˜.

PROBLEMS 32. (a) Each date, 𝑑, has a unique daily snowfall, 𝑆, associated with it. So snowfall is a function of date. (b) On December 12, the snowfall was approximately 5 inches. (c) On December 11, the snowfall was above 10 inches. (d) Looking at the graph we see that the largest increase in the snowfall was between December 10 and December 11. 33. (a) When the car is 5 years old, it is worth $6000. (b) Since the value of the car decreases as the car gets older, this is a decreasing function. A possible graph is in Figure 1.1: 𝑉 (thousand dollars)

(5, 6)

π‘Ž (years)

Figure 1.1 (c) The vertical intercept is the value of 𝑉 when π‘Ž = 0, or the value of the car when it is new. The horizontal intercept is the value of π‘Ž when 𝑉 = 0, or the age of the car when it is worth nothing. 34. (a) The story in (a) matches Graph (IV), in which the person forgot her books and had to return home. (b) The story in (b) matches Graph (II), the flat tire story. Note the long period of time during which the distance from home did not change (the horizontal part). (c) The story in (c) matches Graph (III), in which the person started calmly but sped up later. The first graph (I) does not match any of the given stories. In this picture, the person keeps going away from home, but his speed decreases as time passes. So a story for this might be: I started walking to school at a good pace, but since I stayed up all night studying calculus, I got more and more tired the farther I walked. 35. The year 2018 was 2 years before 2020 so 2018 corresponds to 𝑑 = 2. Thus, an expression that represents the statement is: 𝑓 (2) = 7.088.


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Chapter One /SOLUTIONS 36. The year 2020 was 0 years before 2020 so 2020 corresponds to 𝑑 = 0. Thus, an expression that represents the statement is: 𝑓 (0) meters. 37. The year 1949 was 2020 βˆ’ 1949 = 71 years before 2020 so 1949 corresponds to 𝑑 = 71. Similarly, we see that the year 2000 corresponds to 𝑑 = 20. Thus, an expression that represents the statement is: 𝑓 (71) = 𝑓 (20). 38. The year 2018 was 2 years before 2020 so 2018 corresponds to 𝑑 = 2. Similarly, 𝑑 = 3 corresponds to the year 2017. Thus, 𝑓 (3) and 𝑓 (2) are the average annual sea level values, in meters, in 2017 and 2018, respectively. Because 11 millimeters is the same as 0.011 meters, the average sea level in 2018, 𝑓 (2), is 0.011 less than the sea level in 2017 which is 𝑓 (3). An expression that represents the statement is: 𝑓 (2) = 𝑓 (3) βˆ’ 0.011. Note that there are other possible equivalent expressions, such as: 𝑓 (2) βˆ’ 𝑓 (3) = βˆ’0.011. 39. See Figure 1.2. driving speed

time

Figure 1.2

40. See Figure 1.3. distance driven

time

Figure 1.3

41. See Figure 1.4. distance from exit

time

Figure 1.4


1.1 SOLUTIONS

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42. See Figure 1.5. distance between cars

distance driven

Figure 1.5 43. (a) 𝑓 (30) = 10 means that the value of 𝑓 at 𝑑 = 30 was 10. In other words, the temperature at time 𝑑 = 30 minutes was 10β—¦ C. So, 30 minutes after the object was placed outside, it had cooled to 10 β—¦ C. (b) The intercept π‘Ž measures the value of 𝑓 (𝑑) when 𝑑 = 0. In other words, when the object was initially put outside, it had a temperature of π‘Žβ—¦ C. The intercept 𝑏 measures the value of 𝑑 when 𝑓 (𝑑) = 0. In other words, at time 𝑏 the object’s temperature is 0 β—¦ C. 44. (a) The height of the rock decreases as time passes, so the graph falls as you move from left to right. One possibility is shown in Figure 1.6. 𝑠 (meters)

𝑑 (sec)

Figure 1.6 (b) The statement 𝑓 (7) = 12 tells us that 7 seconds after the rock is dropped, it is 12 meters above the ground. (c) The vertical intercept is the value of 𝑠 when 𝑑 = 0; that is, the height from which the rock is dropped. The horizontal intercept is the value of 𝑑 when 𝑠 = 0; that is, the time it takes for the rock to hit the ground. 45. See Figure 1.7. Distance from Kalamazoo 155 120

start in Chicago

arrive in Kalamazoo

Time arrive in Detroit

Figure 1.7 46. (a) We select two points on the line. Using the values (1992, 6.75) and (2006, 12.25) we have Slope =

million barrels per day 12.25 βˆ’ 6.75 = 0.4 . 2006 βˆ’ 1992 year

(b) With 𝑑 as the year and 𝑓 (𝑑) as the quantity of imports in millions of barrels per day, we have 𝑓 (𝑑) = 6.75 + 0.4(𝑑 βˆ’ 1992). Alternatively, if 𝑑 is the number of years since 1992 and if 𝑓 (𝑑) is the quantity of imports in millions of barrels per day 𝑓 (𝑑) = 6.75 + 0.4𝑑.


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Chapter One /SOLUTIONS (c) We have 6.75 + 0.4𝑑 = 18 𝑑 = 28.125. The model predicts imports will reach 18 million barrels a day in the year 1992 + 28.125 = 2020.125. This prediction could serve as a guideline, but it is very risky to put too much reliance on a prediction more than ten years into the future, especially since there has been a drop in imports since 2008. Many unexpected events could drastically change the economic environment during that time. This prediction should be used with caution. 47. (a) Reading coordinates from the graph, we see that rainfall π‘Ÿ = 100 mm corresponds to about 𝑄 = 600 kgβˆ•hectare, and π‘Ÿ = 600 mm corresponds to about 𝑄 = 5800 kgβˆ•hectare. Using a difference quotient we have Δ𝑄 5800 βˆ’ 600 = = 10.4 kgβˆ•hectare per mm. Ξ”π‘Ÿ 600 βˆ’ 100 (b) Every additional 1 mm of annual rainfall corresponds to an additional 10.4 kg of grass per hectare. (c) Using the slope, we see that the equation has the form Slope =

𝑄 = 𝑏 + 10.4π‘Ÿ. Substituting π‘Ÿ = 100 and 𝑄 = 600 we can solve for 𝑏. 𝑏 + 10.4(100) = 600 𝑏 = βˆ’440. The equation of the line is 𝑄 = βˆ’440 + 10.4π‘Ÿ. 48. (a) Reading coordinates from the graph, we see that rainfall π‘Ÿ = 100 mm corresponds to about 𝑄 = 300 kgβˆ•hectare, and π‘Ÿ = 600 mm corresponds to about 𝑄 = 3200 kgβˆ•hectare. Using a difference quotient we have Δ𝑄 3200 βˆ’ 300 = = 5.8 kgβˆ•hectare per mm. Ξ”π‘Ÿ 600 βˆ’ 100 (b) Every additional 1 mm of annual rainfall corresponds to an additional 5.8 kg of grass per hectare. (c) Using the slope, we see that the equation has the form Slope =

𝑄 = 𝑏 + 5.8π‘Ÿ. Substituting π‘Ÿ = 100 and 𝑄 = 300 we can solve for 𝑏. 𝑏 + 5.8(100) = 300 𝑏 = βˆ’280. The equation of the line is 𝑄 = βˆ’280 + 5.8π‘Ÿ. 49. The difference quotient Ξ”π‘„βˆ•Ξ”π‘Ÿ equals the slope of the line and represents the increase in the quantity of grass per millimeter of rainfall. We see from the graph that the slope of the line for 1939 is larger than the slope of the line for 1997. Thus, each additional 1 mm of rainfall in 1939 led to a larger increase in the quantity of grass than in 1997. 50. (a) Substituting into the function 𝑔(𝑑): 𝑔(10) = 300 + 1.4 β‹… (10) = 314 ppm 𝑔(20) = 300 + 1.4 β‹… (20) = 328 ppm 𝑔(100) = 300 + 1.4 β‹… (100) = 440 ppm (b) Substituting into β„Ž(𝑑): β„Ž(10) = 300 + 1.5 β‹… (10) = 315 ppm β„Ž(20) = 300 + 1.5 β‹… (20) = 330 ppm β„Ž(100) = 300 + 1.5 β‹… (100) = 450 ppm (c) They differ in slope, 1.4 vs. 1.5 ppm per year. This creates a larger difference between 𝑔(𝑑) and β„Ž(𝑑) for larger values of 𝑑: For 𝑑 = 10, the difference is β„Ž(10) βˆ’ 𝑔(10) = 315 βˆ’ 314 = 1 ppm. For 𝑑 = 100, the difference is β„Ž(100) βˆ’ 𝑔(100) = 450 βˆ’ 440 = 10 ppm.


1.1 SOLUTIONS

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51. (a) Let π‘₯ be the average minimum daily temperature (β—¦ C), and let 𝑦 be the date the marmot is first sighted. Reading coordinates from the graph, we see that temperature π‘₯ = 12β—¦ C corresponds to date 𝑦 = 137 days after Jan 1, and π‘₯ = 22β—¦ C corresponds to 𝑦 = 109 days. Using a difference quotient, we have days Δ𝑦 109 βˆ’ 137 = = βˆ’2.8 β—¦ . Ξ”π‘₯ 22 βˆ’ 12 C (b) The slope is negative. An increase in the temperatures corresponds to an earlier sighting of a marmot. Marmots come out of hibernation earlier in years with warmer average daily minimum temperature. (c) We have Δ𝑦 = Slope Γ— Ξ”π‘₯ = (βˆ’2.8)(6) = 16.8 days. β—¦ If temperatures are 6 C higher, then marmots come out of hibernations about 17 days earlier. (d) Using the slope, we see that the equation has the form Slope =

𝑦 = 𝑏 βˆ’ 2.8π‘₯. Substituting π‘₯ = 12 and 𝑦 = 137 we solve for 𝑏. 𝑏 βˆ’ 2.8(12) = 137 𝑏 = 171. The equation of the line is 𝑦 = 171 βˆ’ 2.8π‘₯. 52. (a) If the first date of bare ground is 140, then, according to the figure, the first bluebell flower is sighted about day 150, that is 150 βˆ’ 140 = 10 days later. (b) Let π‘₯ be the first date of bare ground, and let 𝑦 be the date the first bluebell flower is sighted. Reading coordinates from the graph, we see that date π‘₯ = 130 days after Jan 1 corresponds to date 𝑦 = 142 days after Jan 1, and π‘₯ = 170 days corresponds to 𝑦 = 173 days. Using a difference quotient we have Δ𝑦 173 βˆ’ 142 = = 0.775 days per day. Ξ”π‘₯ 170 βˆ’ 130 (c) The slope is positive, so an increase in the π‘₯-variable corresponds to an increase in the 𝑦-variable. These variables represents days in the year, and larger values indicate days that are later in the year. Thus if bare ground first occurs later in the year, then bluebells first flower later in the year. Positive slope means that bluebells flower later when the snow cover lasts longer. (d) Using the slope, we see that the equation has the form Slope =

𝑦 = 𝑏 + 0.775π‘₯. Substituting π‘₯ = 130 and 𝑦 = 142 we can solve for 𝑏. 𝑏 + 0.775(130) = 142 𝑏 = 41.25. The equation of the line is 𝑦 = 41.25 + 0.775π‘₯. 53. (a) We have π‘š =

256 = 14.222 cm per hour. When the snow started, there were 100 cm on the ground, so 18 𝑓 (𝑑) = 100 + 14.222𝑑.

(b) The domain of 𝑓 is 0 ≀ 𝑑 ≀ 18 hours. The range is 100 ≀ 𝑓 (𝑑) ≀ 356 cm. 54. (a) We find the slope π‘š and intercept 𝑏 in the linear equation 𝐢 = 𝑏 + π‘šπ‘€. To find the slope π‘š, we use π‘š=

Δ𝐢 1098.32 βˆ’ 694.55 = = 134.59 dollars per ton. Δ𝑀 8βˆ’5

We substitute to find 𝑏: 𝐢 = 𝑏 + π‘šπ‘€ 694.55 = 𝑏 + (134.59)(5) 𝑏 = 21.6 dollars. The linear formula is 𝐢 = 21.6 + 134.59𝑀. (b) The slope is 134.59 dollars per ton. Each additional ton of waste collected costs $134.59. (c) The intercept is $21.60. The flat fee for waste collection is $21.60. This is the amount charged even if there is no waste.


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Chapter One /SOLUTIONS

55. We are looking for a linear function 𝑦 = 𝑓 (π‘₯) that, given a time π‘₯ in years, gives a value 𝑦 in dollars for the value of the refrigerator. We know that when π‘₯ = 0, that is, when the refrigerator is new, 𝑦 = 950, and when π‘₯ = 7, the refrigerator is worthless, so 𝑦 = 0. Thus (0, 950) and (7, 0) are on the line that we are looking for. The slope is then given by 950 βˆ’7 It is negative, indicating that the value decreases as time passes. Having found the slope, we can take the point (7, 0) and use the point-slope formula: 𝑦 βˆ’ 𝑦1 = π‘š(π‘₯ βˆ’ π‘₯1 ). So, 950 (π‘₯ βˆ’ 7) π‘¦βˆ’0 = βˆ’ 7 950 π‘₯ + 950. 𝑦=βˆ’ 7 π‘š=

55 βˆ’ 40 Ξ”$ = = $0.025/cu. ft. 56. (a) Charge per cubic foot = Ξ” cu. ft. 1600 βˆ’ 1000 Alternatively, if we let 𝑐 = cost, 𝑀 = cubic feet of water, 𝑏 = fixed charge, and π‘š = cost/cubic feet, we obtain 𝑐 = 𝑏 + π‘šπ‘€. Substituting the information given in the problem, we have 40 = 𝑏 + 1000π‘š 55 = 𝑏 + 1600π‘š. Subtracting the first equation from the second yields 15 = 600π‘š, so π‘š = 0.025. (b) The equation is 𝑐 = 𝑏 + 0.025𝑀, so 40 = 𝑏 + 0.025(1000), which yields 𝑏 = 15. Thus the equation is 𝑐 = 15 + 0.025𝑀. (c) We need to solve the equation 100 = 15 + 0.025𝑀, which yields 𝑀 = 3400. It costs $100 to use 3400 cubic feet of water. 57. (a) The first company’s price for a day’s rental with π‘š miles on it is 𝐢1 (π‘š) = 40 + 0.15π‘š. Its competitor’s price for a day’s rental with π‘š miles on it is 𝐢2 (π‘š) = 50 + 0.10π‘š. (b) See Figure 1.8. 𝐢 (cost in dollars) 𝐢1 (π‘š) = 40 + 0.15π‘š

150 100

𝐢2 (π‘š) = 50 + 0.10π‘š

50 0

200

400

600

800

π‘š (miles)

Figure 1.8 (c) To find which company is cheaper, we need to determine where the two lines intersect. We let 𝐢1 = 𝐢2 , and thus 40 + 0.15π‘š = 50 + 0.10π‘š 0.05π‘š = 10 π‘š = 200. If you are going more than 200 miles a day, the competitor is cheaper. If you are going less than 200 miles a day, the first company is cheaper. 58. (a) We find the slope π‘š and intercept 𝑏 in the linear equation 𝑆 = 𝑏 + π‘šπ‘‘. To find the slope π‘š, we use 66 βˆ’ 113 Δ𝑆 = = βˆ’0.94. Δ𝑑 50 βˆ’ 0 When 𝑑 = 0, we have 𝑆 = 113, so the intercept 𝑏 is 113. The linear formula is π‘š=

𝑆 = 113 βˆ’ 0.94𝑑. (b) We use the formula 𝑆 = 113 βˆ’ 0.94𝑑. When 𝑆 = 20, we have 20 = 113 βˆ’ 0.94𝑑 and so 𝑑 = 98.9. If this linear model were correct, the average male sperm count would drop below the fertility level during the year 2038.


1.1 SOLUTIONS

9

59. (a)

(i) 𝑓 (2001) = 272 (ii) 𝑓 (2019) = 607 (b) The average yearly increase is the rate of change. Yearly increase =

𝑓 (2019) βˆ’ 𝑓 (2001) 607 βˆ’ 272 335 = = = 18.611 billionaires per year. 2019 βˆ’ 2001 18 18

So on average, there were between 18 and 19 more billionaires in the US each year. (c) Since we assume the rate of increase remains constant, we use a linear function with slope 335βˆ•18 = 18.611 billionaires per year. The equation is 335 𝑑 𝑓 (𝑑) = 𝑏 + 18 where 𝑓 (2001) = 272, so 335 (2001) 272 = 𝑏 + 18 𝑏 = βˆ’36,968.833. Thus, 𝑓 (𝑑) = 18.611𝑑 βˆ’ 36,968.833. 60. (a) The variable costs for π‘₯ acres are $200π‘₯, or 0.2π‘₯ thousand dollars. The total cost, 𝐢 (again in thousands of dollars), of planting π‘₯ acres is: 𝐢 = 𝑓 (π‘₯) = 10 + 0.2π‘₯. This is a linear function. See Figure 1.9. Since 𝐢 = 𝑓 (π‘₯) increases with π‘₯, 𝑓 is an increasing function of π‘₯. Look at the values of 𝐢 shown in the table; you will see that each time π‘₯ increases by 1, 𝐢 increases by 0.2. Because 𝐢 increases at a constant rate as π‘₯ increases, the graph of 𝐢 against π‘₯ is a line. (b) See Figure 1.9 and Table 1.1. Table 1.1 Cost of planting seed π‘₯

𝐢

0

10

2

10.4

3

10.6

4

10.8

5

11

6

11.2

𝐢 (thosand $) 10

𝐢 = 10 + 0.2π‘₯

5

2

4

6

π‘₯ (acres)

Figure 1.9

(c) The vertical intercept of 10 corresponds to the fixed costs. For 𝐢 = 𝑓 (π‘₯) = 10 + 0.2π‘₯, the intercept on the vertical axis is 10 because 𝐢 = 𝑓 (0) = 10 + 0.2(0) = 10. Since 10 is the value of 𝐢 when π‘₯ = 0, we recognize it as the initial outlay for equipment, or the fixed cost. The slope 0.2 corresponds to the variable costs. The slope is telling us that for every additional acre planted, the costs go up by 0.2 thousand dollars. The rate at which the cost is increasing is 0.2 thousand dollars per acre. Thus the variable costs are represented by the slope of the line 𝑓 (π‘₯) = 10 + 0.2π‘₯. 61. We will let 𝑇 = amount of fuel for take-off, 𝐿 = amount of fuel for landing, 𝑃 = amount of fuel per mile in the air, π‘š = the length of the trip in miles. Then 𝑄, the total amount of fuel needed, is given by 𝑄(π‘š) = 𝑇 + 𝐿 + 𝑃 π‘š.


10

Chapter One /SOLUTIONS

62. (a) The scale of the graph makes it impossible to read values of 𝑓 (423) and 𝑓 (422) accurately enough to evaluate their difference. But that difference equals the slope of the line, which we can estimate. Using the points (400, 2000) and (600, 6000) on the line, we have 6000 βˆ’ 2000 = 20. Slope = 600 βˆ’ 400 Thus 𝑓 (423) βˆ’ 𝑓 (422) = 20. (b) We have Δ𝑦 = Slope Γ— Ξ”π‘₯ = (20)(517 βˆ’ 513) = 80. Thus 𝑓 (517) βˆ’ 𝑓 (513) = 80. 63. (a) The scale of the graph makes it impossible to read values of 𝑔(4210) and 𝑔(4209) accurately enough to evaluate their difference. But that difference equals the slope of the line, which we can estimate. Using the points (3000, 70) and (5000, 50) on the line, we have 50 βˆ’ 70 = βˆ’0.01. Slope = 5000 βˆ’ 3000 So Δ𝑦 = Slope Γ— Ξ”π‘₯ = (βˆ’0.01)(4210 βˆ’ 4209) = βˆ’0.01. Thus 𝑔(4210) βˆ’ 𝑔(4209) = βˆ’0.01. (b) We have Δ𝑦 = Slope Γ— Ξ”π‘₯ = (βˆ’0.01)(3760 βˆ’ 3740) = βˆ’0.2. Thus 𝑔(3760) βˆ’ 𝑔(3740) = βˆ’0.2. 64. (a) From the graph we estimate 𝑉 (1) = 100 mph and 𝑉 (2) = 50 mph. (b) No. Counterexample with 𝑑 = 1: 𝑉 (𝑑 + 1) = 𝑉 (2) = 50 𝑉 (𝑑) + 1 = 𝑉 (1) + 1 = 100 + 1 = 101. (c) No. Counterexample with 𝑑 = 1: 𝑉 (𝑑 + 1) = 50 𝑉 (𝑑) + 𝑉 (1) = 100 + 100 = 200. 65. (a) From the graph we estimate 𝑁(1) = 50% and 𝑁(2) = 75%. (b) No. Counterexample with 𝑑 = 1: 𝑁(𝑑 + 1) = 𝑁(2) = 75 𝑁(𝑑) + 1 = 𝑁(1) + 1 = 50 + 1 = 51. (c) No. Counterexample with 𝑑 = 1: 𝑁(𝑑 + 1) = 75 𝑁(𝑑) + 𝑁(1) = 50 + 50 = 100. 66. (a) The largest time interval was 2016–2018 since the percentage growth rate increased each year from 0.33 to 6.20 to 10.10 from 2016 to 2018. This means US exports of biofuels were growing faster and faster between 2016 and 2018. (Note that the percentage growth rate was a decreasing function of time over 2012–2014 and in 2015–2016.) (b) The largest time interval was 2015–2018 since the percentage growth rates were positive for each of these consecutive years. This means that the amount of biofuels exported from the US steadily increased during the four years from 2015 to 2018, after a large fall in 2014.


1.1 SOLUTIONS

11

67. (a) The largest time interval was 2015–2017 since the percentage growth rate increased each year from 2015 to 2016 to 2017. This means that from 2015 to 2017 the US consumption of hydroelectric power grew relatively more with each successive year. (b) The largest time interval was 2012–2015 since the percentage growth rates were negative for each of these four consecutive years. This means that the amount of hydroelectric power consumed by the US industrial sector steadily decreased during this period. 68. (a) The largest time interval was 2008–2010 since the percentage growth rate decreased each year from 2008 to 2009 to 2010. This means that from 2008 to 2010 the US price per watt of a solar panel fell relatively more with each successive year. (b) The largest time interval was 2009–2010 since the percentage growth rates were negative for each of these two consecutive years. This means that the US price per watt of a solar panel decreased during these two years, after an increase in the previous year. 69. (a) Since 2014 corresponds to 𝑑 = 0, the average annual sea level in Aberdeen in 2014 was 7.071 meters. (b) Looking at the table, we see that the average annual sea level was 7.083 twenty five years before 2014, or in the year 1989. Similar reasoning shows that the average sea level was 6.985 meters 100 years before 2014, or in 1914. (c) Because 1889 was 125 years before 2014, we see that the sea level value corresponding to the year 1889 is 6.900 (this is the sea level value corresponding to 𝑑 = 125). Similar reasoning yields Table 1.2. Table 1.2 Year

1889

1914

1939

1964

1989

2014

𝑆

6.900

6.985

6.964

6.990

7.083

7.071

70. (a) This could be a linear function because 𝑀 increases by 2.7 as β„Ž increases by 4. (b) We find the slope π‘š and the intercept 𝑏 in the linear equation 𝑀 = 𝑏 + π‘šβ„Ž. We first find the slope π‘š using the first two points in the table. Since we want 𝑀 to be a function of β„Ž, we take π‘š=

82.4 βˆ’ 79.7 Δ𝑀 = = 0.68. Ξ”β„Ž 172 βˆ’ 168

Substituting the first point and the slope π‘š = 0.68 into the linear equation 𝑀 = 𝑏+π‘šβ„Ž, we have 79.7 = 𝑏+(0.68)(168), so 𝑏 = βˆ’34.54. The linear function is 𝑀 = 0.68β„Ž βˆ’ 34.54. The slope, π‘š = 0.68, is in units of kg per cm. (c) We find the slope and intercept in the linear function β„Ž = 𝑏 + π‘šπ‘€ using π‘š = Ξ”β„Žβˆ•Ξ”π‘€ to obtain the linear function β„Ž = 1.47𝑀 + 50.79. Alternatively, we could solve the linear equation found in part (b) for β„Ž. The slope, π‘š = 1.47, has units cm per kg. 71. (a) Since the differences in 𝑃 -values are constant (Δ𝑃 = 147) for equally spaced β„Ž-values (Ξ”β„Ž = 2), 𝑃 could be a linear function of β„Ž. (b) To find a formula for 𝑃 = 𝑓 (β„Ž), we first find the slope: Δ𝑃 147 = = 73.5 torr per meter. Δ𝑑 2 Thus, the equation of the line has the form 𝑃 = 73.5β„Ž + 𝑏, where 𝑏 is the vertical intercept. To find 𝑏, we choose a point from the table: for example, when β„Ž = 6, we have 𝑃 = 1201. Substituting these values, we have 𝑃 = 73.5β„Ž + 𝑏 1201 = 73.5(6) + 𝑏 𝑏 = 1201 βˆ’ 73.5(6) = 760. Therefore, 𝑃 = 𝑓 (β„Ž) = 73.5β„Ž + 760. The slope is 73.5 torr per meter which means that the pressure increases by 73.5 torr for each additional meter of depth below the surface of the lake. The vertical intercept is 760 torr, which means that the pressure at the surface of the lake is 760 torr.


12

Chapter One /SOLUTIONS (c) The pressure at the surface of the lake is 𝑓 (0) = 760 torr. Since we want the value of β„Ž when the pressure is twice that at the surface, we solve 𝑓 (β„Ž) = 2 β‹… 760: 2 β‹… 760 = 𝑓 (β„Ž) 1520 = 73.5β„Ž + 760 73.5β„Ž = 760 760 = 10.34. β„Ž= 73.5

72. (a) Since the initial value is $25,000 and the slope is βˆ’2000, the value of the vehicle at time 𝑑 is 𝑉 (𝑑) = 25000 βˆ’ 2000𝑑. The cost of repairs has initial value 0 and slope 1500, so 𝐢(𝑑) = 1500𝑑. Figure 1.10 shows the graphs of these two functions. dollars 25000 𝑉 (𝑑)

20000

𝐢(𝑑)

15000 10000 5000 0

2

4

6

8

10

12

𝑑 (years)

Figure 1.10 (b) The vehicle value equals the repair cost, when 𝑉 (𝑑) = 𝐢(𝑑). 25000 βˆ’ 2000𝑑 = 1500𝑑 25000 = 3500𝑑 7.143 = 𝑑. Thus, replace during the eighth year (because the first year ends at 𝑑 = 1). Since 0.143 years is 0.143(12) = 1.7 months, replacement should take place in the second month of the eighth year. (c) Since 6% of the orginal value is 1500, the vehicle should be replaced when 𝑉 (𝑑) = 1500. 25000 βˆ’ 2000𝑑 = 1500 25000 = 1500 + 2000𝑑 23500 = 2000𝑑 11.750 = 𝑑. Thus, in the twelfth year (because the first year ends at 𝑑 = 1). Since 0.75 years is 9 months, replacement should take place at the end of the ninth month of the twelfth year. 73. (a) If the bakery owner decreases the price, the customers want to buy more. Thus, the slope of 𝑑(π‘ž) is negative. If the owner increases the price, she is willing to make more cakes. Thus the slope of 𝑠(π‘ž) is positive. (b) To determine whether an ordered pair (π‘ž, 𝑝) is a solution to the inequality, we substitute the values of π‘ž and 𝑝 into the inequality and see whether the resulting statement is true. Substituting the two ordered pairs gives (60, 18):

18 ≀ 20 βˆ’ 60βˆ•20, or 18 ≀ 17.

This is false, so (60, 18) is not a solution.

(120, 12): 12 ≀ 20 βˆ’ 120βˆ•20, or 12 ≀ 14. This is true, so (120, 12) is a solution.


1.1 SOLUTIONS

13

The pair (60, 18) is not a solution to the inequality 𝑝 ≀ 20 βˆ’ π‘žβˆ•20. This means that the price $18 is higher than the unit price at which customers would be willing to buy a total of 60 cakes. So customers are not willing to buy 60 cakes at $18. The pair (120, 12) is a solution, meaning that $12 is not more than the price at which customers would be willing to buy 120 cakes. Thus customers are willing to buy a total of 120 (and more) cakes at $12. Each solution (π‘ž, 𝑝) represents a quantity of cakes π‘ž that customers would be willing to buy at the unit price 𝑝. (c) In order to be a solution to both of the given inequalities, a point (π‘ž, 𝑝) must lie on or below the line 𝑝 = 20 βˆ’ π‘žβˆ•20 and on or above the line 𝑝 = 11 + π‘žβˆ•40. Thus, the solution set of the given system of inequalities is the region shaded in Figure 1.11. A point (π‘ž, 𝑝) in this region represents a quantity π‘ž of cakes that customers would be willing to buy, and that the bakery-owner would be willing to make and sell, at the price 𝑝. 𝑝 25 20

𝑑(π‘ž) = 20 βˆ’ π‘žβˆ•20 (120, 14)

15 10

𝑠(π‘ž) = 11 + π‘žβˆ•40

5 40

80

120

160

200

π‘ž

Figure 1.11: Possible cake sales at different prices and quantities (d) To find the rightmost point of this region, we need to find the intersection point of the lines 𝑝 = 20 βˆ’ π‘žβˆ•20 and 𝑝 = 11 + π‘žβˆ•40. At this point, 𝑝 is equal to both 20 βˆ’ π‘žβˆ•20 and 11 + π‘žβˆ•40, so these two expressions are equal to each other: π‘ž π‘ž = 11 + 20 βˆ’ 20 40 π‘ž π‘ž 9= + 20 40 3π‘ž 9= 40 π‘ž = 120. Therefore, π‘ž = 120 is the maximum number of cakes that can be sold at a price at which customers are willing to buy them all, and the owner of the bakery is willing to make them all. The price at this point is 𝑝 = 20 βˆ’ 120βˆ•20 = 14 dollars. (In economics, this price is called the equilibrium price, since at this point there is no incentive for the owner of the bakery to raise or lower the price of the cakes.) = βˆ’1 and 𝑦-intercept 2, so its equation is 74. (a) The line given by (0, 2) and (1, 1) has slope π‘š = 2βˆ’1 βˆ’1 𝑦 = βˆ’π‘₯ + 2. The points of intersection of this line with the parabola 𝑦 = π‘₯2 are given by π‘₯2 = βˆ’π‘₯ + 2 π‘₯2 + π‘₯ βˆ’ 2 = 0 (π‘₯ + 2)(π‘₯ βˆ’ 1) = 0. The solution π‘₯ = 1 corresponds to the point we are already given, so the other solution, π‘₯ = βˆ’2, gives the π‘₯-coordinate of 𝐢. When we substitute back into either equation to get 𝑦, we get the coordinates for 𝐢, (βˆ’2, 4). = 1 βˆ’ 𝑏, and 𝑦-intercept at (0, 𝑏), so we can write the equation (b) The line given by (0, 𝑏) and (1, 1) has slope π‘š = π‘βˆ’1 βˆ’1 for the line as we did in part (a): 𝑦 = (1 βˆ’ 𝑏)π‘₯ + 𝑏. We then solve for the points of intersection with 𝑦 = π‘₯2 the same way: π‘₯2 = (1 βˆ’ 𝑏)π‘₯ + 𝑏 2

π‘₯ βˆ’ (1 βˆ’ 𝑏)π‘₯ βˆ’ 𝑏 = 0 π‘₯2 + (𝑏 βˆ’ 1)π‘₯ βˆ’ 𝑏 = 0 (π‘₯ + 𝑏)(π‘₯ βˆ’ 1) = 0


14

Chapter One /SOLUTIONS Again, we have the solution at the given point (1, 1), and a new solution at π‘₯ = βˆ’π‘, corresponding to the other point of intersection 𝐢. Substituting back into either equation, we can find the 𝑦-coordinate for 𝐢 is 𝑏2 , and thus 𝐢 is given by (βˆ’π‘, 𝑏2 ). This result agrees with the particular case of part (a) where 𝑏 = 2.

75. Looking at the given data, it seems that Galileo’s hypothesis was incorrect. The first table suggests that velocity is not a linear function of distance, since the increases in velocity for each foot of distance are themselves getting smaller. Moreover, the second table suggests that velocity is instead proportional to time, since for each second of time, the velocity increases by 32 ft/sec.

Strengthen Your Understanding 76. The slope of a linear function of π‘₯ is given by the function’s rise (Δ𝑦) over its run (Ξ”π‘₯) over any interval. So, for 𝑦 = 𝑏+π‘šπ‘₯, we have: Δ𝑦 . Slope = π‘š = Ξ”π‘₯ 77. The line π‘₯ = 3 is vertical, so it is not a function of π‘₯: it fails the vertical line test. The line 𝑦 = 3 is horizontal, hence a linear function of π‘₯ with slope 0. 78. The line 𝑦 βˆ’ 3 = 0 or, equivalently, 𝑦 = 3 is horizontal, hence has slope 0 in the π‘₯𝑦-plane. 79. The line 𝑦 = 0.5 βˆ’ 3π‘₯ has a negative slope and is therefore a decreasing function. 80. If 𝑦 is directly proportional to π‘₯ we have 𝑦 = π‘˜π‘₯. Adding the constant 1 to give 𝑦 = 2π‘₯ + 1 means that 𝑦 is not proportional to π‘₯. 81. One possible answer is 𝑓 (π‘₯) = 2π‘₯ + 3. 8 82. One possible answer is π‘ž = 1βˆ•3 . 𝑝 83. False. A line can be put through any two points in the plane. However, if the line is vertical, it is not the graph of a function. 84. True. Suppose we start at π‘₯ = π‘₯1 and increase π‘₯ by 1 unit to π‘₯1 + 1. If 𝑦 = 𝑏 + π‘šπ‘₯, the corresponding values of 𝑦 are 𝑏 + π‘šπ‘₯1 and 𝑏 + π‘š(π‘₯1 + 1). Thus 𝑦 increases by Δ𝑦 = 𝑏 + π‘š(π‘₯1 + 1) βˆ’ (𝑏 + π‘šπ‘₯1 ) = π‘š. 85. True. Solving for 𝑦 on the second equation, we see that the second linear function has the same equation as the first: π‘₯ = βˆ’π‘¦ + 1 π‘₯ βˆ’ 1 = βˆ’π‘¦ βˆ’π‘₯ + 1 = 𝑦. 86. False. Solving for 𝑦 on the second equation, we get 𝑦 = (βˆ’1βˆ•2)π‘₯ + 1 which is a linear function with a different slope and intercept from the first equation. 87. False. For example, let 𝑦 = π‘₯ + 1. Then the points (1, 2) and (2, 3) are on the line. However the ratios 3 2 =2 and = 1.5 1 2 are different. The ratio π‘¦βˆ•π‘₯ is constant for linear functions of the form 𝑦 = π‘šπ‘₯, but not in general. (Other examples are possible.) 88. False. For example, if 𝑦 = 4π‘₯ + 1 (so π‘š = 4) and π‘₯ = 1, then 𝑦 = 5. Increasing π‘₯ by 2 units gives 3, so 𝑦 = 4(3) + 1 = 13. Thus, 𝑦 has increased by 8 units, not 4 + 2 = 6. (Other examples are possible.) √ 89. (b) and (c). For 𝑔(π‘₯) = π‘₯, the domain and range are all nonnegative numbers, and for β„Ž(π‘₯) = π‘₯3 , the domain and range are all real numbers.

Solutions for Section 1.2 EXERCISES 1. The graph shows a concave up function.


1.2 SOLUTIONS

15

2. The graph shows a concave down function. 3. This graph is neither concave up or down. 4. The graph is concave up. 5. Initial quantity = 5; growth rate = 0.07 = 7%. 6. Initial quantity = 7.7; growth rate = βˆ’0.08 = βˆ’8% (decay). 7. Initial quantity = 3.2; growth rate = 0.03 = 3% (continuous). 8. Initial quantity = 15; growth rate = βˆ’0.06 = βˆ’6% (continuous decay). ( )𝑑 9. Since 𝑒0.25𝑑 = 𝑒0.25 β‰ˆ (1.2840)𝑑 , we have 𝑃 = 15(1.2840)𝑑 . This is exponential growth since 0.25 is positive. We can also see that this is growth because 1.2840 > 1. 10. Since π‘’βˆ’0.5𝑑 = (π‘’βˆ’0.5 )𝑑 β‰ˆ (0.6065)𝑑 , we have 𝑃 = 2(0.6065)𝑑 . This is exponential decay since βˆ’0.5 is negative. We can also see that this is decay because 0.6065 < 1. 11. 𝑃 = 𝑃0 (𝑒0.2 )𝑑 = 𝑃0 (1.2214)𝑑 . Exponential growth because 0.2 > 0 or 1.2214 > 1. 12. 𝑃 = 7(π‘’βˆ’πœ‹ )𝑑 = 7(0.0432)𝑑 . Exponential decay because βˆ’πœ‹ < 0 or 0.0432 < 1. 13. (a) Let 𝑄 = 𝑄0 π‘Žπ‘‘ . Then 𝑄0 π‘Ž5 = 75.94 and 𝑄0 π‘Ž7 = 170.86. So 𝑄0 π‘Ž7 170.86 = = 2.25 = π‘Ž2 . 75.94 𝑄0 π‘Ž5 So π‘Ž = 1.5. (b) Since π‘Ž = 1.5, the growth rate is π‘Ÿ = 0.5 = 50%. 14. (a) Let 𝑄 = 𝑄0 π‘Žπ‘‘ . Then 𝑄0 π‘Ž0.02 = 25.02 and 𝑄0 π‘Ž0.05 = 25.06. So 𝑄0 π‘Ž0.05 25.06 = = 1.001 = π‘Ž0.03 . 25.02 𝑄0 π‘Ž0.02 So

100

π‘Ž = (1.001) 3 = 1.05. (b) Since π‘Ž = 1.05, the growth rate is π‘Ÿ = 0.05 = 5%. 15. (a) The function is linear with initial population of 1000 and slope of 50, so 𝑃 = 1000 + 50𝑑. (b) This function is exponential with initial population of 1000 and growth rate of 5%, so 𝑃 = 1000(1.05)𝑑 . 16. (a) This is a linear function with slope βˆ’2 grams per day and intercept 30 grams. The function is 𝑄 = 30 βˆ’ 2𝑑, and the graph is shown in Figure 1.12. 𝑄 (grams)

𝑄 (grams)

30

30 𝑄 = 30 βˆ’ 2𝑑

15

Figure 1.12

𝑄 = 30(0.88)𝑑

𝑑 (days)

15

𝑑 (days)

Figure 1.13

(b) Since the quantity is decreasing by a constant percent change, this is an exponential function with base 1βˆ’0.12 = 0.88. The function is 𝑄 = 30(0.88)𝑑 , and the graph is shown in Figure 1.13. 17. The function is increasing and concave up between 𝐷 and 𝐸, and between 𝐻 and 𝐼. It is increasing and concave down between 𝐴 and 𝐡, and between 𝐸 and 𝐹 . It is decreasing and concave up between 𝐢 and 𝐷, and between 𝐺 and 𝐻. Finally, it is decreasing and concave down between 𝐡 and 𝐢, and between 𝐹 and 𝐺 18. (a) It was decreasing from March 2 to March 5 and increasing from March 5 to March 9. (b) From March 5 to 8, the average temperature increased, but the rate of increase went down, from 12β—¦ between March 5 and 6 to 4β—¦ between March 6 and 7 to 2β—¦ between March 7 and 8. From March 7 to 9, the average temperature increased, and the rate of increase went up, from 2β—¦ between March 7 and 8 to 9β—¦ between March 8 and 9.


16

Chapter One /SOLUTIONS

PROBLEMS 19. (a) A linear function must change by exactly the same amount whenever π‘₯ changes by some fixed quantity. While β„Ž(π‘₯) decreases by 3 whenever π‘₯ increases by 1, 𝑓 (π‘₯) and 𝑔(π‘₯) fail this test, since both change by different amounts between π‘₯ = βˆ’2 and π‘₯ = βˆ’1 and between π‘₯ = βˆ’1 and π‘₯ = 0. So the only possible linear function is β„Ž(π‘₯), so it will be given by a formula of the type: β„Ž(π‘₯) = π‘šπ‘₯ + 𝑏. As noted, π‘š = βˆ’3. Since the 𝑦-intercept of β„Ž is 31, the formula for β„Ž(π‘₯) is β„Ž(π‘₯) = 31 βˆ’ 3π‘₯. (b) An exponential function must grow by exactly the same factor whenever π‘₯ changes by some fixed quantity. Here, 𝑔(π‘₯) increases by a factor of 1.5 whenever π‘₯ increases by 1. Since the 𝑦-intercept of 𝑔(π‘₯) is 36, 𝑔(π‘₯) has the formula 𝑔(π‘₯) = 36(1.5)π‘₯ . The other two functions are not exponential; β„Ž(π‘₯) is not because it is a linear function, and 𝑓 (π‘₯) is not because it both increases and decreases. 20. Table A and Table B could represent linear functions of π‘₯. Table A could represent the constant linear function 𝑦 = 2.2 because all 𝑦 values are the same. Table B could represent a linear function of π‘₯ with slope equal to 11βˆ•4. This is because π‘₯ values that differ by 4 have corresponding 𝑦 values that differ by 11, and π‘₯ values that differ by 8 have corresponding 𝑦 values that differ by 22. In Table C, 𝑦 decreases and then increases as π‘₯ increases, so the table cannot represent a linear function. Table D does not show a constant rate of change, so it cannot represent a linear function. 21. Table D is the only table that could represent an exponential function of π‘₯. This is because, in Table D, the ratio of 𝑦 values is the same for all equally spaced π‘₯ values. Thus, the 𝑦 values in the table have a constant percent rate of decrease: 4.5 2.25 9 = = = 0.5. 18 9 4.5 Table A represents a constant function of π‘₯, so it cannot represent an exponential function. In Table B, the ratio between 𝑦 values corresponding to equally spaced π‘₯ values is not the same. In Table C, 𝑦 decreases and then increases as π‘₯ increases. So neither Table B nor Table C can represent exponential functions. 22. Since 𝑓 is linear, its slope is a constant π‘š=

20 βˆ’ 10 = 5. 2βˆ’0

Thus 𝑓 increases 5 units for unit increase in π‘₯, so 𝑓 (1) = 15,

𝑓 (3) = 25,

𝑓 (4) = 30.

Since 𝑔 is exponential, its growth factor is constant. Writing 𝑔(π‘₯) = π‘Žπ‘π‘₯ , we have 𝑔(0) = π‘Ž = 10, so 𝑔(π‘₯) = 10 β‹… 𝑏π‘₯ . Since 𝑔(2) = 10 β‹… 𝑏2 = 20, we have 𝑏2 = 2 and since 𝑏 > 0, we have √ 𝑏 = 2. √ Thus 𝑔 increases by a factor of 2 for unit increase in π‘₯, so √ √ √ 𝑔(1) = 10 2, 𝑔(3) = 10( 2)3 = 20 2,

√ 𝑔(4) = 10( 2)4 = 40.

Notice that the value of 𝑔(π‘₯) doubles between π‘₯ = 0 and π‘₯ = 2 (from 𝑔(0) = 10 to 𝑔(2) = 20), so the doubling time of 𝑔(π‘₯) is 2. Thus, 𝑔(π‘₯) doubles again between π‘₯ = 2 and π‘₯ = 4, confirming that 𝑔(4) = 40. 23. We see that 1.09 β‰ˆ 1.03, and therefore β„Ž(𝑠) = 𝑐(1.03)𝑠 ; 𝑐 must be 1. Similarly 2.42 = 1.1, and so 𝑓 (𝑠) = π‘Ž(1.1)𝑠 ; π‘Ž = 2. 1.06 2.20 Lastly, 3.65 β‰ˆ 1.05, so 𝑔(𝑠) = 𝑏(1.05)𝑠 ; 𝑏 β‰ˆ 3. 3.47

24. (a) This is the graph of a linear function, which increases at a constant rate, and thus corresponds to π‘˜(𝑑), which increases by 0.3 over each interval of 1. (b) This graph is concave down, so it corresponds to a function whose increases are getting smaller, as is the case with β„Ž(𝑑), whose increases are 10, 9, 8, 7, and 6. (c) This graph is concave up, so it corresponds to a function whose increases are getting bigger, as is the case with 𝑔(𝑑), whose increases are 1, 2, 3, 4, and 5. 25. (a) This is a linear function, corresponding to 𝑔(π‘₯), whose rate of decrease is constant, 0.6. (b) This graph is concave down, so it corresponds to a function whose rate of decrease is increasing, like β„Ž(π‘₯). (The rates are βˆ’0.2, βˆ’0.3, βˆ’0.4, βˆ’0.5, βˆ’0.6.) (c) This graph is concave up, so it corresponds to a function whose rate of decrease is decreasing, like 𝑓 (π‘₯). (The rates are βˆ’10, βˆ’9, βˆ’8, βˆ’7, βˆ’6.)


1.2 SOLUTIONS

17

26. Graph (I) and (II) are of increasing functions, therefore the growth factor for both functions is greater than 1. Since graph (I) increases faster than graph (II), graph (I) corresponds to the larger growth factor. Therefore graph (I) matches 𝑄 = 50(1.4)𝑑 and graph (II) is 𝑄 = 50(1.2)𝑑 . Similarly, since graphs (III) and (IV) are both of decreasing functions, they have growth factors between 0 and 1. Since graph (IV) decreases faster than graph (III), graph (IV) has the smaller decay factor. Thus graph (III) is 𝑄 = 50(0.8)𝑑 and graph (IV) is 𝑄 = 50(0.6)𝑑 . 27. We look for an equation of the form 𝑦 = 𝑦0 π‘Žπ‘₯ since the graph looks exponential. The points (0, 3) and (2, 12) are on the graph, so 3 = 𝑦0 π‘Ž0 = 𝑦0 and

12 = 𝑦0 β‹… π‘Ž2 = 3 β‹… π‘Ž2 ,

giving

π‘Ž = Β±2.

π‘₯

Since π‘Ž > 0, our equation is 𝑦 = 3(2 ). 28. We look for an equation of the form 𝑦 = 𝑦0 π‘Žπ‘₯ since the graph looks exponential. The points (0, 18) and (2, 8) are on the graph, so 18 = 𝑦0 π‘Ž0 = 𝑦0 √

and 2

2

8 = 𝑦0 β‹… π‘Ž = 18 β‹… π‘Ž ,

giving

𝑦 = 18

( )π‘₯ 2 . 3

Since π‘Ž > 0, our equation is

π‘Ž=Β±

4 . 9

29. We look for an equation of the form 𝑦 = 𝑦0 π‘Žπ‘₯ since the graph looks exponential. The points (1, 6) and (2, 18) are on the graph, so 6 = 𝑦0 π‘Ž1 and 18 = 𝑦0 π‘Ž2 18 = 3, and so 6 = 𝑦0 π‘Ž = 𝑦0 β‹… 3; thus, 𝑦0 = 2. Hence 𝑦 = 2(3π‘₯ ). 6 30. The graphs looks like that of an exponential function that has been shifted down by 2 units since it appears that it has horizontal asymptote 𝑦 = βˆ’2. Therefore we are looking for an equation of the form 𝑦 = π‘Žπ‘π‘₯ βˆ’ 2. Since at π‘₯ = 0 we have 𝑦 = 8 = π‘Ž βˆ’ 2, giving π‘Ž = 10. The point (1, 4) is on the graph, so 4 = 10𝑏1 βˆ’ 2, giving 𝑏 = 106 = 35 . Therefore, ( )π‘₯ 3 βˆ’ 2. 𝑦 = 10 5 𝑦 π‘Ž2

Therefore π‘Ž = 𝑦0 π‘Ž = 0

31. We look for an equation of the form 𝑦 = 𝑦0 π‘Žπ‘₯ since the graph looks exponential. The points (βˆ’1, 8) and (1, 2) are on the graph, so 8 = 𝑦0 π‘Žβˆ’1 and 2 = 𝑦0 π‘Ž1 Therefore

𝑦 π‘Žβˆ’1 8 1 = 0 = 2 , giving π‘Ž = 12 , and so 2 = 𝑦0 π‘Ž1 = 𝑦0 β‹… 12 , so 𝑦0 = 4. 2 ( )𝑦0 π‘Ž π‘Ž

Hence 𝑦 = 4

1 2

π‘₯

.

32. The difference, 𝐷, between the horizontal asymptote and the graph appears to decrease exponentially, so we look for an equation of the form 𝐷 = 𝐷0 π‘Žπ‘₯ where 𝐷0 = 4 = difference when π‘₯ = 0. Since 𝐷 = 4 βˆ’ 𝑦, we have 4 βˆ’ 𝑦 = 4π‘Žπ‘₯ or 𝑦 = 4 βˆ’ 4π‘Žπ‘₯ = 4(1 βˆ’ π‘Žπ‘₯ ) The point (1, 2) is on the graph, so 2 = 4(1 βˆ’ π‘Ž1 ), giving π‘Ž = 12 . Therefore 𝑦 = 4(1 βˆ’ ( 12 )π‘₯ ).

33. (a) See Figure 1.14. (b) No. The points in the plot do not lie even approximately on a straight line, so a linear model is a poor choice. (c) No. The plot shows that 𝐻 is a decreasing function of π‘Œ that might be leveling off to an asymptote at 𝐻 = 0. These are features of an exponential decay function, but their presence does not show that 𝐻 is an exponential function of π‘Œ . We can do a more precise check by dividing each value of 𝐻 by the previous year’s 𝐻.


18

Chapter One /SOLUTIONS 13 million Houses in 2011 = = 0.710 Houses in 2010 18.3 million 7.8 million Houses in 2012 = = 0.600 Houses in 2011 13 million 3.9 million Houses in 2013 = = 0.500 Houses in 2012 7.8 million Houses in 2014 1 million = = 0.256 Houses in 2013 3.9 million Houses in 2015 0.5 million = = 0.500. Houses in 2014 1 million If 𝐻 were an exponential function of π‘Œ , the ratios would be approximately constant. Since they are not approximately constant, we see that an exponential model is a poor choice. 𝐻 20 15 10 5 2010 2011 2012 2013 2014 2015

π‘Œ

Figure 1.14 34. (a) See Figure 1.15. customers

time

Figure 1.15 (b) β€œThe rate at which new people try it” is the rate of change of the total number of people who have tried the product. Thus, the statement of the problem is telling you that the graph is concave downβ€”the slope is positive but decreasing, as the graph shows. 35. (a) Advertising is generally cheaper in bulk; spending more money will give better and better marginal results initially, (Spending $5,000 could give you a big newspaper ad reaching 200,000 people; spending $100,000 could give you a series of TV spots reaching 50,000,000 people.) See Figure 1.16. (b) The temperature of a hot object decreases at a rate proportional to the difference between its temperature and the temperature of the air around it. Thus, the temperature of a very hot object decreases more quickly than a cooler object. The graph is decreasing and concave up. See Figure 1.17 (We are assuming that the coffee is all at the same temperature.) temperature

revenue

advertising

Figure 1.16

time

Figure 1.17


1.2 SOLUTIONS

19

36. (a) We have 𝑃0 = 1 million, and π‘˜ = 0.02, so 𝑃 = (1,000,000)(𝑒0.02𝑑 ). (b) 𝑃

1,000,000 𝑑

37. If production continues to decay exponentially at a continuous rate of 9.1% per year, the production 𝑓 (𝑑) at time 𝑑 years after 2008 is 𝑓 (𝑑) = 84π‘’βˆ’0.091𝑑 . In 2025, production is predicted to be 𝑓 (17) = 84π‘’βˆ’0.091(17) = 17.882 million barrels per day. 38. (a) Let 𝑃 represent the population of the world (in billions), and let 𝑑 represent the number of years since 2017. Then we have 𝑃 = 7.41(1.011)𝑑 . (b) According to this formula, the population of the world in the year 2025 (at 𝑑 = 8) will be 𝑃 = 7.41(1.011)8 = 8.09 billion people. (c) The graph is shown in Figure 1.18. The population of the world has doubled when 𝑃 = 14.82; we see on the graph that this occurs at approximately 𝑑 = 63.4. Under these assumptions, the doubling time of the world’s population is about 63.4 years. 𝑃 (billion people) 14.82 7.41 𝑑 (years)

63.4

Figure 1.18

39. (a) Since the population was 2.7 million in 2010, and 𝑑 is measured since 2010 so 𝑑 = 0 in 2010, we have 𝑁0 = 2.7. Then 𝑁 = 3.0 when 𝑑 = 8, so 3 = 2.7π‘Ž8 ) ( 3 1βˆ•8 π‘Ž= = 1.0133. 2.7 Thus,

𝑁 = 2.7(1.0133)𝑑 .

(b) In 2000, we have 𝑑 = βˆ’10, so 𝑁 = 2.7

((

3 2.7

)1βˆ•8 )βˆ’10

= 2.367 million.

40. Direct calculation reveals that each 1000 foot increase in altitude results in a longer takeoff roll by a factor of about 1.096. Since the value of 𝑑 when β„Ž = 0 (sea level) is 𝑑 = 670, we are led to the formula 𝑑 = 670(1.096)β„Žβˆ•1000 , where 𝑑 is the takeoff roll, in feet, and β„Ž is the airport’s elevation, in feet.


20

Chapter One /SOLUTIONS Alternatively, we can write

𝑑 = 𝑑0 π‘Žβ„Ž ,

where 𝑑0 is the sea level value of 𝑑, 𝑑0 = 670. In addition, when β„Ž = 1000, 𝑑 = 734, so 734 = 670π‘Ž1000 . Solving for π‘Ž gives π‘Ž= so

(

734 670

)1βˆ•1000

= 1.00009124,

𝑑 = 670(1.00009124)β„Ž .

41. Since we are told that the rate of decay is continuous, we use the function 𝑄(𝑑) = 𝑄0 π‘’π‘Ÿπ‘‘ to model the decay, where 𝑄(𝑑) is the amount of strontium-90 which remains at time 𝑑, and 𝑄0 is the original amount. Then 𝑄(𝑑) = 𝑄0 π‘’βˆ’0.0247𝑑 . So after 100 years, and

𝑄(100) = 𝑄0 π‘’βˆ’0.0247β‹…100 𝑄(100) = π‘’βˆ’2.47 β‰ˆ 0.0846 𝑄0

so about 8.46% of the strontium-90 remains. 42. (a) Since 𝑦 is the number of US colonies, we need a growth factor smaller than 1 in order to describe a colony loss. A loss of 18.9% per year means a yearly growth factor equal to 1 βˆ’ 0.189 = 0.811. An annual percentage loss smaller than 18.9% would still be sustainable, and would result in a growth factor larger than 0.811 but still smaller than 1. Hence, II is the only function that could describe an economically sustainable colony loss trend. (b) Function I says the number of US bee colonies is growing by 18.9% a year. Function II says bee colony loss is 10.9% per year. Function III indicates a bee colony loss of 20.2% a year. 43. (a) Since 2𝑓 (𝑑) = 6π‘’π‘˜π‘‘ and 𝑔(𝑑) = π‘Žπ‘’2π‘˜π‘‘ , we cannot find a value of π‘Ž that makes these functions equal. (b) Since (𝑓 (𝑑))2 = (3π‘’π‘˜π‘‘ )2 = 9𝑒2π‘˜π‘‘ , we can arrange that 𝑔(𝑑) = (𝑓 (𝑑))2 if π‘Žπ‘’2π‘˜π‘‘ = 9𝑒2π‘˜π‘‘ π‘Ž = 9.

44. The doubling time 𝑑 depends only on the growth rate; it is the solution to 2 = (1.02)𝑑 , since 1.02𝑑 represents the factor by which the population has grown after time 𝑑. Trial and error shows that (1.02)35 β‰ˆ 1.9999 and (1.02)36 β‰ˆ 2.0399, so that the doubling time is about 35 years. 45. (a) Since sales of electronic devices doubled in 12 years, sales in 1997 were 438βˆ•2 = 219 million devices. Because part (b) asks for the annual percentage growth rate (not a continuous growth rate), we use an exponential function of the form 𝑆(𝑑) = 𝑆0 𝑏𝑑 , where 𝑏 is the annual growth factor. We have 438 = 219𝑏12 , so 2 = 𝑏12 and 𝑏 = 21βˆ•12 = 1.05946. Thus, 𝑆(𝑑) = 219(1.05946)𝑑 . (b) The annual growth rate was 5.946%.


1.2 SOLUTIONS

21

46. (a) Because the population is growing exponentially, the time it takes to double is the same, regardless of the population levels we are considering. For example, the population is 20,000 at time 3.7, and 40,000 at time 6.0. This represents a doubling of the population in a span of 6.0 βˆ’ 3.7 = 2.3 years. How long does it take the population to double a second time, from 40,000 to 80,000? Looking at the graph once again, we see that the population reaches 80,000 at time 𝑑 = 8.3. This second doubling has taken 8.3 βˆ’ 6.0 = 2.3 years, the same amount of time as the first doubling. Further comparison of any two populations on this graph that differ by a factor of two will show that the time that separates them is 2.3 years. Similarly, during any 2.3 year period, the population will double. Thus, the doubling time is 2.3 years. (b) Suppose 𝑃 = 𝑃0 π‘Žπ‘‘ doubles from time 𝑑 to time 𝑑+𝑑. We now have 𝑃0 π‘Žπ‘‘+𝑑 = 2𝑃0 π‘Žπ‘‘ , so 𝑃0 π‘Žπ‘‘ π‘Žπ‘‘ = 2𝑃0 π‘Žπ‘‘ . Thus, canceling 𝑃0 and π‘Žπ‘‘ , 𝑑 must be the number such that π‘Žπ‘‘ = 2, no matter what 𝑑 is. 47. (a) After 50 years, the amount of money is

𝑃 = 2𝑃0 .

After 100 years, the amount of money is 𝑃 = 2(2𝑃0 ) = 4𝑃0 . After 150 years, the amount of money is 𝑃 = 2(4𝑃0 ) = 8𝑃0 . (b) The amount of money in the account doubles every 50 years. Thus in 𝑑 years, the balance doubles π‘‘βˆ•50 times, so 𝑃 = 𝑃0 2π‘‘βˆ•50 . 48. (a) Since 162.5 = 325βˆ•2, there are 162.5 mg remaining after 𝐻 hours. Since 81.25 = 162.5βˆ•2, there are 81.25 mg remaining 𝐻 hours after there were 162.5 mg, so 2𝐻 hours after there were 325 mg. Since 40.625 = 81.25βˆ•2, there are 41.625 mg remaining 𝐻 hours after there were 81.25 mg, so 3𝐻 hours after there were 325 mg. (b) Each additional 𝐻 hours, the quantity is halved. Thus in 𝑑 hours, the quantity was halved π‘‘βˆ•π» times, so 𝐴 = 325

( )π‘‘βˆ•π» 1 . 2

49. (a) The quantity of radium decays exponentially, so we know 𝑄 = 𝑄0 π‘Žπ‘‘ . When 𝑑 = 1620, we have 𝑄 = 𝑄0 βˆ•2 so 𝑄0 = 𝑄0 π‘Ž1620 . 2 Thus, canceling 𝑄0 , we have 1 2 ( )1βˆ•1620 1 π‘Ž= = 0.999572 2

π‘Ž1620 =

Thus the formula is 𝑄 = 𝑄0 (0.999572)𝑑 . (b) After 500 years, Fraction remaining =

1 β‹… 𝑄0 (0.999572)500 = 0.80731. 𝑄0

so 80.731% is left. 50. Let 𝑄0 be the initial quantity absorbed in 1960. Then the quantity, 𝑄, of strontium-90 left after 𝑑 years is 𝑄 = 𝑄0

( )π‘‘βˆ•29 1 . 2

Since 2010 βˆ’ 1960 = 50 years, in 2010 Fraction remaining =

( )50βˆ•29 ( )50βˆ•29 1 1 1 β‹… 𝑄0 = = 0.30268 = 30.268%. 𝑄0 2 2


22

Chapter One /SOLUTIONS

51. The half-life of cesium-137 is the time it takes for the original sample of 10 grams to decay to 5 grams, so we must find 𝑑 such that 𝑓 (𝑑) = 5. We have 10(1βˆ•2)π‘‘βˆ•30 = 5 (1βˆ•2)π‘‘βˆ•30 = 1βˆ•2 𝑑 =1 30 𝑑 = 30, so the half-life is 30 years. To find the continuous rate of decay, observe that 𝑓 (𝑑) = 10(1βˆ•2)π‘‘βˆ•30 = 10(𝑒ln(1βˆ•2) )π‘‘βˆ•30 = 10𝑒𝑑 ln(1βˆ•2)βˆ•30 = 10π‘’βˆ’0.02310𝑑 , so the continuous decay rate is 2.31% per year. 52. (a) The 1.109 represents the number of food parcels, in millions, when 𝑑 = 0. Approximately 1,109,000 food parcels were supplied in 2015. (b) The continuous growth rate is 0.12, or 12%, per year. (c) Since 𝑒0.12𝑑 = (𝑒0.12 )𝑑 = 1.127𝑑 , we see that the annual growth factor is 1.127. Thus, the annual growth rate is 1.127βˆ’1 = 0.127 = 12.7% per year. (d) Since the annual growth factor is only 1.127, the number of food parcels does not double each year. The doubling time is more than one year. 53. The graph shows the concentration leveling off to π‘Ž. (a) The value of π‘Ž represents the value at which the concentration levels off. (b) We see π‘Ž is positive. (c) At 𝑑 = 0, we have 𝑓 (0) = π‘Ž βˆ’ π‘π‘’π‘˜β‹…0 = π‘Ž βˆ’ 𝑏. Since the graph goes through the origin, 𝑓 (0) = 0. Thus π‘Ž βˆ’ 𝑏 = 0 so π‘Ž = 𝑏. (d) Since the concentration of 𝑓 levels off to π‘Ž and 𝑓 (𝑑) = π‘Ž βˆ’ π‘π‘’π‘˜π‘‘ , the term π‘π‘’π‘˜π‘‘ must decay to zero. To make the term π‘π‘’π‘˜π‘‘ decay to zero, π‘˜ must be negative. 54. (a) The function 𝑓 appears to be exponential because ratios of successive output values of π‘ž are approximately equal for equally spaced 𝑑-values; that is 36.4 28.3 22.1 46.7 = = = β‰ˆ 0.78. 60 46.7 36.4 28.3 This tells us that at the end of each second, the remaining charge is 0.78 times the charge at the start of that second. Since the initial charge on the capacitor is 60 πœ‡C, we can approximate by π‘ž = 𝑓 (𝑑) = 60(0.78)𝑑 . (b) We want to solve for 𝑑 at which there is 30 πœ‡C (half the original 60) remaining: 30 = 𝑓 (𝑑) 30 = 60(0.78)𝑑 1 = 0.78𝑑 2 ln(1βˆ•2) = 𝑑 ln(0.78) ln(1βˆ•2) = 2.790. 𝑑= ln(0.78) Therefore, it takes about 2.79 seconds for the charge remaining on the capacitor to be half its initial value. (c) Since 𝑓 (𝑑) = 60(0.78)𝑑 = 60(𝑒ln(0.78) )𝑑 = 60𝑒𝑑 ln(0.78) = 60π‘’βˆ’0.248𝑑 , we see that the continuous rate of decay of the charge on the capacitor is about 25% per second. 55. (a) Since atmospheric pressure at ground level is 760 torr, we know that if 𝑝 = 𝑓 (β„Ž), then 𝑓 (0) = 760. This means 𝑓 (β„Ž) has the form 𝑓 (β„Ž) = 760 β‹… π‘β„Ž . We are also given that 𝑓 (5.6) = 341, so 760 β‹… 𝑏5.6 = 341 341 𝑏5.6 = 760 ) ( 341 1βˆ•5.6 𝑏= = 0.86666. 760


1.2 SOLUTIONS Therefore,

23

𝑝 = 𝑓 (β„Ž) = 760(0.867)β„Ž .

(b) From part (a), we have 𝑏 = 0.86666 = 1 + π‘Ÿ, which means that π‘Ÿ = 0.86666 βˆ’ 1 = βˆ’0.13334. Therefore, the atmospheric pressure decreases by about 13.334% for each 1 km increase in elevation. (c) To find the elevation where atmospheric pressure is 100 torr, we set 𝑓 (β„Ž) = 100 and solve: 𝑓 (β„Ž) = 100 760(0.86666)β„Ž = 100 100 0.86666β„Ž = 760 ) ( 100 β„Ž ln(0.86666) = ln 760 ln(100βˆ•760) β„Ž= = 14.172 km. ln(0.86666) 56. (a) Since the annual growth factor from 2012 to 2013 was 1 + (58.95βˆ•100) = 1.5895 and 899(1.5895) = 1428.961, the US consumed about 1429 million gallons of biodiesel in 2013. Since the annual growth factor from 2013 to 2014 was 1 + (βˆ’0.0084) = 0.9916 and 1428.961(0.9916) = 1416.96, the US consumed approximately 1417 million gallons of biodiesel in 2014. (b) Completing the table of annual consumption of biodiesel and plotting the data gives Figure 1.19. Table 1.3 Year

2012

2013

2014

2015

2016

2017

2018

Consumption of biodiesel (mn gal)

899

1429

1417

1494

2085

1985

1896

consumption of biodiesel (mn gal) 2500 2000 1500 1000 500

2012

2014

2016

2018

year

Figure 1.19 57. (a) False, because the annual percent growth is not constant over this interval. (b) (i) The US consumption of biodiesel grew by more that 58% in 2013. (ii) The US consumption of biodiesel fell by 4.8% in 2017. 58. (a) Since the annual growth factor from 2013 to 2014 was 1 βˆ’ 0.0342 = 0.9658 and 2.686 β‹… 0.9658 = 2.5941, the US generated approximately 2.6 quadrillion BTUs of hydroelectric power in 2014. Since the annual growth factor from 2014 to 2015 was 1 βˆ’ 0.0397 = 0.9603 and 2.5941(1 βˆ’ 0.0397) = 2.4911, the US generated about 2.5 quadrillion BTUs of hydroelectric power in 2015. (b) Completing the table of annual consumption of hydroelectric power and plotting the data gives Figure 1.20. Year Generation of hydro. power (quadrillion BTU)

2013

2014

2015

2016

2017

2018

2.686

2.594

2.491

2.678

3.004

2.918

(c) The largest increase in the US generation of hydroelectric power occurred in 2017. In this year, the US generation of hydroelectric power increased by about 326 trillion BTUs to 3.004 quadrillion BTUs, up from 2.678 quadrillion BTUs in 2016.


24

Chapter One /SOLUTIONS consumption of hydro. power (quadillion BTU) 3.5 3 2.5

2014

2016

2018

year

Figure 1.20 59. (a) From Figure 1.41 in the text, we can see the approximate percent growth for each year over the previous year: Year

2013

2014

2015

2016

2017

2018

% growth over previous yr

20

8

3

18

12

8

Since the annual growth factor from 2013 to 2014 was 1 + 0.08 = 1.08 and 1601(1 + 0.08) = 1729.08, the US consumed approximately 1729 trillion BTUs of wind power energy in 2014. Since the annual growth factor from 2014 to 2015 was 1 + 0.03 = 1.03 and 1729.08(1 + 0.03) = 1780.95, the US consumed about 1781 trillion BTUs of wind power energy in 2015. (b) Completing the table of annual consumption of wind power and plotting the data gives Figure 1.21. Year

2013

2014

2015

2016

2017

2018

Consumption of wind power (trillion BTU)

1601

1729

1781

2102

2354

2542

(c) The largest increase in the US consumption of wind power energy occurred in 2016. In this year the US consumption of wind power energy rose by about 321 trillion BTUs to 2102 trillion BTUs, up from 1781 trillion BTUs in 2015. consumption of wind power energy (trillion BTU) 2500 2250 2000 1750 1500 2014

2016

2018

year

Figure 1.21 60. (a) The US consumption of wind power energy increased by at least 10% in 2013, 2016 and in 2017, relative to the previous year. Consumption did not decrease during the time period shown because all the annual percent growth values are positive, indicating a steady increase in the US consumption of wind power energy between 2013 and 2018. (b) True. From the figure we see that consumption increased by about 18% during 2016, by about 12% during 2017, and by about 12% during 2018. This means that π‘₯(1 + 0.18) units of wind power energy were consumed in 2016 if π‘₯ had been consumed in 2015. Similarly, π‘₯(1 + 0.18)(1 + 0.12) units of wind power energy were consumed in 2017 if π‘₯ had been consumed in 2015, and π‘₯(1 + 0.18)(1 + 0.12)(1 + 0.08) units of wind power energy were consumed in 2018 if π‘₯ had been consumed in 2015. Since π‘₯(1 + 0.18)(1 + 0.12)(1 + 0.08) = π‘₯(1.4273) = π‘₯(1 + 0.4273), wind power consumption was about 42.73% greater in 2018 than in 2015. Thus, consumption of wind power energy grew by about 42.73% from the beginning of 2015 to the end of 2018. Note that adding these three percentages would be only 38%, however there is a multiplier effect which makes the change more than 40%.


1.2 SOLUTIONS

25

61. (a) Since the 𝑦-intercept of each graph is above the π‘₯-axis, we know that π‘Ž, 𝑐, and 𝑝 must all be positive. (b) Since the graph of 𝑦 = π‘Žπ‘π‘₯ is increasing and goes through (1, 1), the 𝑦-intercept, π‘Ž, must be less than 1. Since the 𝑦-intercept is positive, we know that 0 < π‘Ž < 1. Since 𝑦 = 𝑐𝑑 π‘₯ and 𝑦 = π‘π‘ž π‘₯ are both decreasing, both 𝑑 and π‘ž must be between 0 and 1. (c) The graphs of 𝑦 = 𝑐𝑑 π‘₯ and 𝑦 = π‘π‘ž π‘₯ have the same 𝑦-intercepts, therefore we have 𝑐 = 𝑝. (d) Since the point (1, 1) lies on the graph of 𝑦 = π‘Žπ‘π‘₯ , we know that 1 = π‘Žπ‘1 . Therefore, π‘Ž and 𝑏 are reciprocals of each other. Similarly, 𝑝 and π‘ž are reciprocals of each other.

Strengthen Your Understanding 62. A quantity that doubles daily has a daily growth factor of 2, and a daily growth rate of 100%. 63. The function 𝑦 = π‘’βˆ’0.25π‘₯ is decreasing but its graph is concave up. 64. The graph of 𝑦 = 2π‘₯ is a straight line and is neither concave up or concave down. 65. The last two points are not on the graph of 𝑒π‘₯ . Points of the graph of this function have the form (π‘₯, 𝑒π‘₯ ). The values π‘₯ = 2 and π‘₯ = 3 correspond to the points (2, 𝑒2 ) and (3, 𝑒3 ). 66. The functions 𝑦 = π‘’βˆ’π‘‘ and 𝑦 = (0.9)𝑑 , for example, are both decreasing but have a vertical intercept of 1. To get a vertical intercept of πœ‹ we must get this value when evaluating at 𝑑 = 0. Hence, two possible functions are 𝑦 = πœ‹π‘’βˆ’π‘‘ and 𝑦 = πœ‹(0.9)𝑑 . 67. One possible answer is π‘ž = 2.2(0.97)𝑑 . 68. One possible answer is 𝑓 (π‘₯) = 2(1.1)π‘₯ . 69. One possibility is 𝑦 = π‘’βˆ’π‘₯ βˆ’ 5. 70. Any exponential function of the form 𝑦 = π‘Žπ‘₯ , where 1 < π‘Ž < 𝑒 works. A possible example is 𝑦 = 2π‘₯ . 71. True. Using algebra and rules of exponents, we can rewrite 𝑓 (π‘₯) so that it has the form 𝑃0 π‘’π‘˜π‘₯ : 𝑓 (π‘₯) = 𝑒2π‘₯ βˆ•(2𝑒5π‘₯ ) 1 = 𝑒2π‘₯βˆ’5π‘₯ 2 1 βˆ’3π‘₯ = 𝑒 . 2

72. False. The 𝑦-intercept is 𝑦 = 2 + 3π‘’βˆ’0 = 5. 73. True, since, as 𝑑 β†’ ∞, we know π‘’βˆ’4𝑑 β†’ 0, so 𝑦 = 5 βˆ’ 3π‘’βˆ’4𝑑 β†’ 5. 74. False. Suppose 𝑦 = 5π‘₯ . Then increasing π‘₯ by 1 increases 𝑦 by a factor of 5. However increasing π‘₯ by 2 increases 𝑦 by a factor of 25, not 10, since 𝑦 = 5π‘₯+2 = 5π‘₯ β‹… 52 = 25 β‹… 5π‘₯ . (Other examples are possible.) 75. True. Suppose 𝑦 = 𝐴𝑏π‘₯ and we start at the point (π‘₯1 , 𝑦1 ), so 𝑦1 = 𝐴𝑏π‘₯1 . Then increasing π‘₯1 by 1 gives π‘₯1 + 1, so the new 𝑦-value, 𝑦2 , is given by 𝑦2 = 𝐴𝑏π‘₯1 +1 = 𝐴𝑏π‘₯1 𝑏 = (𝐴𝑏π‘₯1 )𝑏, so 𝑦2 = 𝑏𝑦1 . Thus, 𝑦 has increased by a factor of 𝑏, so 𝑏 = 3, and the function is 𝑦 = 𝐴3π‘₯ . However, if π‘₯1 is increased by 2, giving π‘₯1 + 2, then the new 𝑦-value, 𝑦3 , is given by 𝑦3 = 𝐴3π‘₯1 +2 = 𝐴3π‘₯1 32 = 9𝐴3π‘₯1 = 9𝑦1 . Thus, 𝑦 has increased by a factor of 9. 76. True. For example, 𝑓 (π‘₯) = (0.5)π‘₯ is an exponential function which decreases. (Other examples are possible.) 77. True. If 𝑏 > 1, then π‘Žπ‘π‘₯ β†’ 0 as π‘₯ β†’ βˆ’βˆž. If 0 < 𝑏 < 1, then π‘Žπ‘π‘₯ β†’ 0 as π‘₯ β†’ ∞. In either case, the function 𝑦 = π‘Ž + π‘Žπ‘π‘₯ has 𝑦 = π‘Ž as the horizontal asymptote. 78. True, since π‘’βˆ’π‘˜π‘‘ β†’ 0 as 𝑑 β†’ ∞, so 𝑦 β†’ 20 as 𝑑 β†’ ∞.


Chapter One /SOLUTIONS

26

Solutions for Section 1.3 EXERCISES 1.

𝑦

(a)

𝑦

(b)

4

4

βˆ’2

2

π‘₯

𝑦

π‘₯

βˆ’2

βˆ’2

π‘₯

𝑦

(c)

2

π‘₯

βˆ’2

βˆ’4 𝑦

4

π‘₯

βˆ’2

4

2

βˆ’4

π‘₯

𝑦

(f)

4

2

2

βˆ’4 𝑦

(e)

π‘₯

4

βˆ’2

βˆ’4

2

βˆ’4

4

2

βˆ’4

π‘₯

𝑦

(b) 4

βˆ’2

2

βˆ’4 𝑦

(d)

4

βˆ’2

βˆ’4

π‘₯

𝑦

(f)

4

2

2

βˆ’4 𝑦

(e)

βˆ’2

(a)

2

βˆ’2

π‘₯

βˆ’4

4

2.

4

βˆ’2

βˆ’4 (d)

𝑦

(c)

π‘₯

βˆ’2

2

βˆ’4

π‘₯


1.3 SOLUTIONS 3.

𝑦

(a)

𝑦

(b) 4

βˆ’2

4

2

π‘₯

2

π‘₯

βˆ’2

2

βˆ’4 𝑦

(e)

𝑦

(f)

4

2

π‘₯

4

βˆ’2

βˆ’4

π‘₯

βˆ’4 𝑦

4

βˆ’2

4

βˆ’2

βˆ’4 (d)

𝑦

(c)

2

π‘₯

βˆ’2

βˆ’4

βˆ’4

4. This graph is the graph of π‘š(𝑑) shifted upward by two units. See Figure 1.22. 4 𝑛(𝑑)

βˆ’4

4

6

𝑑

βˆ’4

Figure 1.22 5. This graph is the graph of π‘š(𝑑) shifted to the right by one unit. See Figure 1.23. 𝑦 4

𝑝(𝑑) βˆ’4

4

βˆ’4

Figure 1.23

2

6

𝑑

π‘₯

27


28

Chapter One /SOLUTIONS 6. This graph is the graph of π‘š(𝑑) shifted to the left by 1.5 units. See Figure 1.24. 4

π‘˜(𝑑)

βˆ’4

4

𝑑

6

βˆ’4

Figure 1.24 7. This graph is the graph of π‘š(𝑑) shifted to the right by 0.5 units and downward by 2.5 units. See Figure 1.25. 4

βˆ’4

𝑑

6 𝑀(𝑑) βˆ’4

Figure 1.25 8. Figure 1.26 shows the appropriate graphs. Note that asymptotes are shown as dashed lines and π‘₯- or 𝑦-intercepts are shown as filled circles. 𝑦

(a)

𝑦

(b)

5

4 𝑦=3

2

2

βˆ’5 βˆ’3

2

5 𝑦

(c)

βˆ’5 βˆ’3

π‘₯

2

π‘₯

βˆ’2 𝑦

(d)

5

5

5 𝑦=4 2

2

1 βˆ’10

βˆ’6

βˆ’1

2

π‘₯ βˆ’5

Figure 1.26 9. (a) 𝑓 (𝑔(1)) = 𝑓 (1 + 1) = 𝑓 (2) = 22 = 4 (b) 𝑔(𝑓 (1)) = 𝑔(12 ) = 𝑔(1) = 1 + 1 = 2 (c) 𝑓 (𝑔(π‘₯)) = 𝑓 (π‘₯ + 1) = (π‘₯ + 1)2 (d) 𝑔(𝑓 (π‘₯)) = 𝑔(π‘₯2 ) = π‘₯2 + 1 (e) 𝑓 (𝑑)𝑔(𝑑) = 𝑑2 (𝑑 + 1)

βˆ’1

2

5

π‘₯


1.3 SOLUTIONS √ √ 2 10. (a) 𝑓 (𝑔(1)) = 𝑓 (1 = 5 √ ) = 𝑓 (1) = √ 1 + 4 √ 2 (b) 𝑔(𝑓 (1)) = 𝑔( 1 + 4) √ = 𝑔( 5) = ( 5) = 5 2 2 (c) 𝑓 (𝑔(π‘₯)) = 𝑓 (π‘₯ √ ) = π‘₯ +√4 (d) 𝑔(𝑓 (π‘₯)) = 𝑔(√ π‘₯ + 4) = ( √π‘₯ + 4)2 = π‘₯ + 4 (e) 𝑓 (𝑑)𝑔(𝑑) = ( 𝑑 + 4)𝑑2 = 𝑑2 𝑑 + 4 11. (a) 𝑓 (𝑔(1)) = 𝑓 (12 ) = 𝑓 (1) = 𝑒1 = 𝑒 (b) 𝑔(𝑓 (1)) = 𝑔(𝑒1 ) = 𝑔(𝑒) = 𝑒2 2 (c) 𝑓 (𝑔(π‘₯)) = 𝑓 (π‘₯2 ) = 𝑒π‘₯ (d) 𝑔(𝑓 (π‘₯)) = 𝑔(𝑒π‘₯ ) = (𝑒π‘₯ )2 = 𝑒2π‘₯ (e) 𝑓 (𝑑)𝑔(𝑑) = 𝑒𝑑 𝑑2 12. (a) 𝑓 (𝑔(1)) = 𝑓 (3 β‹… 1 + 4) = 𝑓 (7) =

1 7

(b) 𝑔(𝑓 (1)) = 𝑔(1βˆ•1) = 𝑔(1) = 7 1 (c) 𝑓 (𝑔(π‘₯)) = 𝑓 (3π‘₯ + 4) = 3π‘₯ ( )+ 4 ( ) 3 1 1 =3 +4= +4 (d) 𝑔(𝑓 (π‘₯)) = 𝑔 π‘₯ π‘₯ π‘₯ 1 4 (e) 𝑓 (𝑑)𝑔(𝑑) = (3𝑑 + 4) = 3 + 𝑑 𝑑 13. We have, for π‘₯ > 0 𝑓 (𝑔(π‘₯)) βˆ’ 𝑔(𝑓 (π‘₯)) = 14. We have,

15. We have,

(√ )2 √ π‘₯ βˆ’ π‘₯2 = π‘₯ βˆ’ π‘₯ = 0.

𝑓 (𝑔(π‘₯)) βˆ’ 𝑔(𝑓 (π‘₯)) = 3(2π‘₯) βˆ’ 2(3π‘₯) = 0.

𝑓 (𝑔(π‘₯)) βˆ’ 𝑔(𝑓 (π‘₯)) = 3(2π‘₯) + 1 βˆ’ 2(3π‘₯ + 1) = 6π‘₯ + 1 βˆ’ 6π‘₯ βˆ’ 2 = βˆ’1.

16. We have,

2

2

𝑓 (𝑔(π‘₯)) βˆ’ 𝑔(𝑓 (π‘₯)) = (𝑒π‘₯ )2 βˆ’ 𝑒π‘₯ = 𝑒2π‘₯ βˆ’ 𝑒π‘₯ .

This cannot be simplified. 17. (a) 𝑓 (𝑑 + 1) = (𝑑 + 1)2 + 1 = 𝑑2 + 2𝑑 + 1 + 1 = 𝑑2 + 2𝑑 + 2. (b) 𝑓 (𝑑2 + 1) = (𝑑2 + 1)2 + 1 = 𝑑4 + 2𝑑2 + 1 + 1 = 𝑑4 + 2𝑑2 + 2. (c) 𝑓 (2) = 22 + 1 = 5. (d) 2𝑓 (𝑑) = 2(𝑑2 + 1) = 2𝑑2 + 2. ( )2 (e) (𝑓 (𝑑))2 + 1 = 𝑑2 + 1 + 1 = 𝑑4 + 2𝑑2 + 1 + 1 = 𝑑4 + 2𝑑2 + 2. 18. (a) 𝑔(2 + β„Ž) = (2 + β„Ž)2 + 2(2 + β„Ž) + 3 = 4 + 4β„Ž + β„Ž2 + 4 + 2β„Ž + 3 = β„Ž2 + 6β„Ž + 11. (b) 𝑔(2) = 22 + 2(2) + 3 = 4 + 4 + 3 = 11, which agrees with what we get by substituting β„Ž = 0 into (a). (c) 𝑔(2 + β„Ž) βˆ’ 𝑔(2) = (β„Ž2 + 6β„Ž + 11) βˆ’ (11) = β„Ž2 + 6β„Ž. 19. π‘š(𝑧 + 1) βˆ’ π‘š(𝑧) = (𝑧 + 1)2 βˆ’ 𝑧2 = 2𝑧 + 1. 20. π‘š(𝑧 + β„Ž) βˆ’ π‘š(𝑧) = (𝑧 + β„Ž)2 βˆ’ 𝑧2 = 2π‘§β„Ž + β„Ž2 . 21. π‘š(𝑧) βˆ’ π‘š(𝑧 βˆ’ β„Ž) = 𝑧2 βˆ’ (𝑧 βˆ’ β„Ž)2 = 2π‘§β„Ž βˆ’ β„Ž2 . 22. π‘š(𝑧 + β„Ž) βˆ’ π‘š(𝑧 βˆ’ β„Ž) = (𝑧 + β„Ž)2 βˆ’ (𝑧 βˆ’ β„Ž)2 = 𝑧2 + 2β„Žπ‘§ + β„Ž2 βˆ’ (𝑧2 βˆ’ 2β„Žπ‘§ + β„Ž2 ) = 4β„Žπ‘§. 23.

𝑓 (βˆ’π‘₯) = (βˆ’π‘₯)6 + (βˆ’π‘₯)3 + 1 = π‘₯6 βˆ’ π‘₯3 + 1. Since 𝑓 (βˆ’π‘₯) β‰  𝑓 (π‘₯) and 𝑓 (βˆ’π‘₯) β‰  βˆ’π‘“ (π‘₯), this function is neither even nor odd.

24.

𝑓 (βˆ’π‘₯) = (βˆ’π‘₯)3 + (βˆ’π‘₯)2 + (βˆ’π‘₯) = βˆ’π‘₯3 + π‘₯2 βˆ’ π‘₯. Since 𝑓 (βˆ’π‘₯) β‰  𝑓 (π‘₯) and 𝑓 (βˆ’π‘₯) β‰  βˆ’π‘“ (π‘₯), this function is neither even nor odd.

25. Since we see 𝑓 is even

𝑓 (βˆ’π‘₯) = (βˆ’π‘₯)4 βˆ’ (βˆ’π‘₯)2 + 3 = π‘₯4 βˆ’ π‘₯2 + 3 = 𝑓 (π‘₯),

29


30

Chapter One /SOLUTIONS

26. Since

𝑓 (βˆ’π‘₯) = (βˆ’π‘₯)3 + 1 = βˆ’π‘₯3 + 1,

we see 𝑓 (βˆ’π‘₯) β‰  𝑓 (π‘₯) and 𝑓 (βˆ’π‘₯) β‰  βˆ’π‘“ (π‘₯), so 𝑓 is neither even nor odd 27. Since

𝑓 (βˆ’π‘₯) = 2(βˆ’π‘₯) = βˆ’2π‘₯ = βˆ’π‘“ (π‘₯),

we see 𝑓 is odd. 28. Since

2

2

𝑓 (βˆ’π‘₯) = 𝑒(βˆ’π‘₯) βˆ’1 = 𝑒π‘₯ βˆ’1 = 𝑓 (π‘₯),

we see 𝑓 is even. 29. Since

𝑓 (βˆ’π‘₯) = (βˆ’π‘₯)((βˆ’π‘₯)2 βˆ’ 1) = βˆ’π‘₯(π‘₯2 βˆ’ 1) = βˆ’π‘“ (π‘₯),

we see 𝑓 is odd 30. Since

𝑓 (βˆ’π‘₯) = π‘’βˆ’π‘₯ + π‘₯,

we see 𝑓 (βˆ’π‘₯) β‰  𝑓 (π‘₯) and 𝑓 (βˆ’π‘₯) β‰  βˆ’π‘“ (π‘₯), so 𝑓 is neither even nor odd 31. The function is not invertible since there are many horizontal lines which hit the function twice. 32. The function is not invertible since there are horizontal lines which hit the function more than once. 33. Since a horizontal line cuts the graph of 𝑓 (π‘₯) = π‘₯2 + 3π‘₯ + 2 two times, 𝑓 is not invertible. See Figure 1.27. 𝑦 4

𝑓 (π‘₯) = π‘₯2 + 3π‘₯ + 2

𝑦 = 2.5

3 2

π‘₯

βˆ’3

Figure 1.27 34. Since a horizontal line cuts the graph of 𝑓 (π‘₯) = π‘₯3 βˆ’ 5π‘₯ + 10 three times, 𝑓 is not invertible. See Figure 1.28. 𝑦

𝑓 (π‘₯) = π‘₯3 βˆ’ 5π‘₯ + 10

10 𝑦=8 π‘₯ -2

2 Figure 1.28


1.3 SOLUTIONS

31

35. Since any horizontal line cuts the graph once, 𝑓 is invertible. See Figure 1.29. 𝑦 𝑓 (π‘₯) = π‘₯3 + 5π‘₯ + 10

40

𝑦 = 30 20 -2

2 π‘₯ 𝑦 = βˆ’19

Figure 1.29 36. (a) 𝑓 (25) is π‘ž corresponding to 𝑝 = 25, or, in other words, the number of items sold when the price is 25. (b) 𝑓 βˆ’1 (30) is 𝑝 corresponding to π‘ž = 30, or the price at which 30 units will be sold. 37. (a) 𝑓 (10,000) represents the value of 𝐢 corresponding to 𝐴 = 10,000, or in other words the cost of building a 10,000 square-foot store. (b) 𝑓 βˆ’1 (20,000) represents the value of 𝐴 corresponding to 𝐢 = 20,000, or the area in square feet of a store which would cost $20,000 to build. 38. 𝑓 βˆ’1 (75) is the length of the column of mercury in the thermometer when the temperature is 75β—¦ F. 39. (a) The equation is 𝑦 = 2π‘₯2 + 1. Note that its graph is narrower than the graph of 𝑦 = π‘₯2 which appears in gray. See Figure 1.30. 8

𝑦 = 2π‘₯2 + 1

6 4

𝑦 = π‘₯2

2

Figure 1.30

8 7 6 5 4 3 2 1

𝑦 = 2(π‘₯2 + 1)

𝑦 = π‘₯2

Figure 1.31

(b) 𝑦 = 2(π‘₯2 + 1) moves the graph up one unit and then stretches it by a factor of two. See Figure 1.31. (c) No, the graphs are not the same. Since 2(π‘₯2 + 1) = (2π‘₯2 + 1) + 1, the second graph is always one unit higher than the first.

PROBLEMS 40. Since 𝑄 = 𝑆 βˆ’ π‘†π‘’βˆ’π‘˜π‘‘ , the graph of 𝑄 is the reflection of 𝑦 about the 𝑑-axis moved up by 𝑆 units. 41. This looks like a shift of the graph 𝑦 = βˆ’π‘₯2 . The graph of 𝑦 = βˆ’π‘₯2 is shifted to the left 1 unit and up 3 units, so a possible formula is 𝑦 = βˆ’(π‘₯ + 1)2 + 3. The graph of 𝑦 = βˆ’π‘₯2 is the graph of 𝑦 = π‘₯2 reflected in the π‘₯-axis. 42. This looks like a shift of the graph 𝑦 = π‘₯3 . The graph is shifted to the right 2 units and down 1 unit, so a possible formula is 𝑦 = (π‘₯ βˆ’ 2)3 βˆ’ 1. 43. We have 𝑣(10) = 65 but the graph of 𝑒 only enables us to evaluate 𝑒(π‘₯) for 0 ≀ π‘₯ ≀ 50. There is not enough information to evaluate 𝑒(𝑣(10)).


32

Chapter One /SOLUTIONS

44. We have approximately 𝑣(40) = 15 and 𝑒(15) = 18 so 𝑒(𝑣(40)) = 18. 45. We have approximately 𝑒(10) = 13 and 𝑣(13) = 60 so 𝑣(𝑒(10)) = 60. 46. We have 𝑒(40) = 60 but the graph of 𝑣 only enables us to evaluate 𝑣(π‘₯) for 0 ≀ π‘₯ ≀ 50. There is not enough information to evaluate 𝑣(𝑒(40)). 47. 𝑓 (𝑔(1)) = 𝑓 (2) β‰ˆ 0.4. 48. 𝑔(𝑓 (2)) β‰ˆ 𝑔(0.4) β‰ˆ 1.1. 49. 𝑓 (𝑓 (1)) β‰ˆ 𝑓 (βˆ’0.4) β‰ˆ βˆ’0.9. 50. Computing 𝑓 (𝑔(π‘₯)) as in Problem 47, we get Table 1.4. From it we graph 𝑓 (𝑔(π‘₯)) in Figure 1.32. Table 1.4 π‘₯

𝑔(π‘₯)

𝑓 (𝑔(π‘₯))

βˆ’3

0.6

βˆ’0.5

βˆ’2.5

βˆ’1.1

βˆ’1.3

βˆ’2

βˆ’1.9

βˆ’1.2

βˆ’1.5

βˆ’1.9

βˆ’1.2 βˆ’1.3

βˆ’1

βˆ’1.4

βˆ’0.5

βˆ’0.5

βˆ’1

0

0.5

βˆ’0.6

0.5

1.4

βˆ’0.2

3

𝑓 (𝑔(π‘₯)) π‘₯ 3

βˆ’3

1

2

0.4

1.5

2.2

0.5

2

1.6

0

2.5

0.1

βˆ’0.7

βˆ’3

3

βˆ’2.5

0.1

Figure 1.32

51. Using the same way to compute 𝑔(𝑓 (π‘₯)) as in Problem 48, we get Table 1.5. Then we can plot the graph of 𝑔(𝑓 (π‘₯)) in Figure 1.33. Table 1.5 π‘₯

𝑓 (π‘₯)

𝑔(𝑓 (π‘₯))

βˆ’3

3

βˆ’2.6

βˆ’2.5

0.1

0.8

βˆ’2

βˆ’1

βˆ’1.4

βˆ’1.5

βˆ’1.3

βˆ’1.8

βˆ’1

βˆ’1.2

βˆ’1.7

βˆ’0.5

βˆ’1

βˆ’1.4

0

βˆ’0.8

βˆ’1

0.5

βˆ’0.6

βˆ’0.6

1

βˆ’0.4

βˆ’0.3

1.5

βˆ’0.1

0.3

3

βˆ’3

𝑔(𝑓 (π‘₯))

3

2

0.3

1.1

2.5

0.9

2

βˆ’3

3

1.6

2.2

Figure 1.33

π‘₯

52. Using the same way to compute 𝑓 (𝑓 (π‘₯)) as in Problem 49, we get Table 1.6. Then we can plot the graph of 𝑓 (𝑓 (π‘₯)) in Figure 1.34.


1.3 SOLUTIONS

33

Table 1.6 π‘₯

𝑓 (π‘₯)

𝑓 (𝑓 (π‘₯))

βˆ’3

3

1.6

βˆ’2.5

0.1

βˆ’0.7

βˆ’2

βˆ’1

βˆ’1.2

βˆ’1.5

βˆ’1.3

βˆ’1.3

βˆ’1

βˆ’1.2

βˆ’1.3

βˆ’0.5

βˆ’1

βˆ’1.2

0

βˆ’0.8

βˆ’1.1

0.5

βˆ’0.6

βˆ’1

3 𝑓 (𝑓 (π‘₯))

βˆ’3

3

1

βˆ’0.4

βˆ’0.9

1.5

βˆ’0.1

βˆ’0.8

2

0.3

βˆ’0.6

2.5

0.9

βˆ’0.4

βˆ’3

3

1.6

0

Figure 1.34

53. 𝑓 (π‘₯) = π‘₯3 ,

π‘₯

𝑔(π‘₯) = π‘₯ + 1.

54. 𝑓 (π‘₯) = π‘₯ + 1, 𝑔(π‘₯) = π‘₯3 . √ 55. 𝑓 (π‘₯) = π‘₯, 𝑔(π‘₯) = π‘₯2 + 4 56. 𝑓 (π‘₯) = 𝑒π‘₯ ,

𝑔(π‘₯) = 2π‘₯

57. The tree has 𝐡 = 𝑦 βˆ’ 1 branches on average and each branch has 𝑛 = 2𝐡 2 βˆ’ 𝐡 = 2(𝑦 βˆ’ 1)2 βˆ’ (𝑦 βˆ’ 1) leaves on average. Therefore Average number of leaves = 𝐡𝑛 = (𝑦 βˆ’ 1)(2(𝑦 βˆ’ 1)2 βˆ’ (𝑦 βˆ’ 1)) = 2(𝑦 βˆ’ 1)3 βˆ’ (𝑦 βˆ’ 1)2 . 58. The volume, 𝑉 , of the balloon is 𝑉 = 43 πœ‹π‘Ÿ3 . When 𝑑 = 3, the radius is 10 cm. The volume is then 𝑉 =

4 4000πœ‹ πœ‹(103 ) = cm3 . 3 3

59. Since 𝑓 is even, we know that 𝑓 (π‘₯) = π‘₯. Since 𝑔 is odd, we know that 𝑔(π‘₯) = βˆ’π‘₯. Since β„Ž(π‘₯) = 𝑔(𝑓 (π‘₯) and 𝑔(π‘₯) is odd, we know that β„Ž(π‘₯) = βˆ’π‘“ (π‘₯), and since 𝑓 (π‘₯) = π‘₯, we know that β„Ž(π‘₯) = βˆ’π‘₯. Using this, we fill in Table 1.7. Table 1.7 π‘₯

𝑓 (π‘₯)

𝑔(π‘₯)

β„Ž(π‘₯)

βˆ’3

0

0

0

βˆ’2

2

2

βˆ’2

βˆ’1

2

2

βˆ’2

0

0

0

0

1

2

βˆ’2

βˆ’2

2

2

βˆ’2

βˆ’2

3

0

0

0

π‘₯

3

βˆ’7

19

4

178

2

1

𝑓 βˆ’1 (π‘₯)

1

2

3

4

5

6

7

60. Values of 𝑓 βˆ’1 are as follows

The domain of 𝑓 βˆ’1 is the set consisting of the integers {3, βˆ’7, 19, 4, 178, 2, 1}.


34

Chapter One /SOLUTIONS

61. (a) We find 𝑓 βˆ’1 (2) by finding the π‘₯ value corresponding to 𝑓 (π‘₯) = 2. Looking at the graph, we see that 𝑓 βˆ’1 (2) = βˆ’1. (b) We construct the graph of 𝑓 βˆ’1 (π‘₯) by reflecting the graph of 𝑓 (π‘₯) over the line 𝑦 = π‘₯. The graphs of 𝑓 βˆ’1 (π‘₯) and 𝑓 (π‘₯) are shown together in Figure 1.35. 𝑦 4 𝑓 (π‘₯) βˆ’4

6

π‘₯

𝑓 βˆ’1 (π‘₯) βˆ’4

Figure 1.35

62. 𝑓 is an increasing function since the amount of fuel used increases as flight time increases. Therefore 𝑓 is invertible. 63. Not invertible. Given a certain number of customers, say 𝑓 (𝑑) = 1500, there could be many times, 𝑑, during the day at which that many people were in the store. So we don’t know which time instant is the right one. 64. Probably not invertible. Since your calculus class probably has less than 363 students, there will be at least two days in the year, say π‘Ž and 𝑏, with 𝑓 (π‘Ž) = 𝑓 (𝑏) = 0. Hence we don’t know what to choose for 𝑓 βˆ’1 (0). 65. Not invertible, since it costs the same to mail a 50-gram letter as it does to mail a 51-gram letter. 66. The carbon footprint, in kilograms of GHGs, of a water bottle that has traveled 150 km from its production source. 67. The carbon footprint of a water bottle that travels 8700 km from its production source is 250 grams of GHGs. 68. The distance from its production source, in km, traveled by a water bottle whose carbon footprint is 1.1 kilograms of GHGs. 69. The combined carbon footprint, in kilograms of GHGs, of a water bottle that has traveled 150 km from its production source and one that has remained at the source. 70. The average per-kilometer increase in the carbon footprint of a water bottle, when the bottle travels between 150 and 1500 km from its production source. 71. The volume of the balloon 𝑑 minutes after inflation began is: 𝑔(𝑓 (𝑑)) ft3 . 72. The volume of the balloon if its radius were twice as big is: 𝑔(2π‘Ÿ) ft3 . 73. The time elapsed is: 𝑓 βˆ’1 (30) min. 74. The time elapsed is: 𝑓 βˆ’1 (𝑔 βˆ’1 (10,000)) min. 75. (a) The function 𝑓 tells us 𝐢 in terms of π‘ž. To get its inverse, we want π‘ž in terms of 𝐢, which we find by solving for π‘ž: 𝐢 = 100 + 2π‘ž, 𝐢 βˆ’ 100 = 2π‘ž, 𝐢 βˆ’ 100 π‘ž= = 𝑓 βˆ’1 (𝐢). 2 (b) The inverse function tells us the number of articles that can be produced for a given cost. 76. (a) Yes, 𝑓 is invertible, since 𝑓 is increasing everywhere. (b) The number 𝑓 βˆ’1 (400) is the year in which 400 million motor vehicles were registered in the world. From the picture, we see that 𝑓 βˆ’1 (400) is around 1979. (c) Since the graph of 𝑓 βˆ’1 is the reflection of the graph of 𝑓 over the line 𝑦 = π‘₯, we get Figure 1.36.


1.3 SOLUTIONS

35

(year) ’10 ’05 ’00 ’95 ’90 ’85 ’80 ’75 ’70 ’65

200

400

600

800

1000

(millions)

Figure 1.36: Graph of 𝑓 βˆ’1

77. (a) The graph shows that 𝑓 (15) is approximately 48. So, the place to find find 15 million-year-old rock is about 48 meters below the Atlantic sea floor. (b) Since 𝑓 is increasing (not decreasing, since the depth axis is reversed!), 𝑓 is invertible. To confirm, notice that the graph of 𝑓 is cut by a horizontal line at most once. (c) Look at where the horizontal line through 120 intersects the graph of 𝑓 and read downward: 𝑓 βˆ’1 (120) is about 35. In practical terms, this means that at a depth of 120 meters down, the rock is 35 million years old. (d) First, we standardize the graph of 𝑓 so that time and depth are increasing from left to right and bottom to top. Points (𝑑, 𝑑) on the graph of 𝑓 correspond to points (𝑑, 𝑑) on the graph of 𝑓 βˆ’1 . We can graph 𝑓 βˆ’1 by taking points from the original graph of 𝑓 , reversing their coordinates, and connecting them. This amounts to interchanging the 𝑑 and 𝑑 axes, thereby reflecting the graph of 𝑓 about the line bisecting the 90β—¦ angle at the origin. Figure 1.37 is the graph of 𝑓 βˆ’1 . (Note that we cannot find the graph of 𝑓 βˆ’1 by flipping the graph of 𝑓 about the line 𝑑 = 𝑑 in because 𝑑 and 𝑑 have different scales in this instance.)

𝑓 βˆ’1

30

100

Time

Depth 𝑓 (standardized)

10

20 10

Time

30 20

Figure 1.37: Graph of 𝑓 , reflected to give that of 𝑓

Depth

100

βˆ’1

78. (a) For positive π‘₯, we have π‘₯ step(π‘₯) = π‘₯ and for negative π‘₯ we have π‘₯ step(π‘₯) = 0. The formula describes the ramp function. (b) For positive π‘₯, we have step(π‘₯) βˆ’ step(βˆ’π‘₯) = 1 βˆ’ 0 = 1, and for negative π‘₯ we have step(π‘₯) βˆ’ step(βˆ’π‘₯) = 0 βˆ’ 1 = βˆ’1. The formula describes the sign function. (c) For positive π‘₯, we have π‘₯ step(π‘₯) βˆ’ π‘₯ step(βˆ’π‘₯) = π‘₯ βˆ’ 0 = π‘₯, and for negative π‘₯ we have π‘₯ step(π‘₯) βˆ’ π‘₯ step(βˆ’π‘₯) = 0 βˆ’ π‘₯ = βˆ’π‘₯. The formula describes the absolute value function.

Strengthen Your Understanding 79. The graph of 𝑓 (π‘₯) = βˆ’(π‘₯ + 1)3 is the graph of 𝑔(π‘₯) = βˆ’π‘₯3 shifted left by 1 unit. 80. The graphs of inverse functions are symmetric with respect to the line 𝑦 = π‘₯. Graphing these two functions for π‘₯ > 0, we see that they are both concave up on the first quadrant, and hence not symmetric with respect to the line 𝑦 = π‘₯. 81. Since 𝑓 (𝑔(π‘₯)) = 3(βˆ’3π‘₯ βˆ’ 5) + 5 = βˆ’9π‘₯ βˆ’ 10, we see that 𝑓 and 𝑔 are not inverse functions.


36

Chapter One /SOLUTIONS

82. Two inverse functions must equal the identity function when composed with each other. This is not true in this case: π‘₯

𝑓 (𝑓 (π‘₯)) = 𝑓 (𝑒π‘₯ ) = 𝑒𝑒 = (𝑒𝑒 )π‘₯ β‰ˆ (15.154)π‘₯ β‰  π‘₯. 83. While 𝑦 = 1βˆ•π‘₯ is sometimes referred to as the multiplicative inverse of π‘₯, the inverse of 𝑓 is 𝑓 βˆ’1 (π‘₯) = π‘₯. 84. One possible answer is 𝑔(π‘₯) = 3 + π‘₯. (There are many answers.) 85. One possibility is 𝑓 (π‘₯) = π‘₯2 + 2. 86. Let 𝑓 (π‘₯) = 3π‘₯, then 𝑓 βˆ’1 (π‘₯) = π‘₯βˆ•3. Then for π‘₯ > 0, we have 𝑓 (π‘₯) > 𝑓 βˆ’1 (π‘₯). 87. We have

𝑔(π‘₯) = 𝑓 (π‘₯ + 2)

because the graph of 𝑔 is obtained by moving the graph of 𝑓 to the left by 2 units. We also have 𝑔(π‘₯) = 𝑓 (π‘₯) + 3 because the graph of 𝑔 is obtained by moving the graph of 𝑓 up by 3 units. Thus, we have 𝑓 (π‘₯ + 2) = 𝑓 (π‘₯) + 3. The graph of 𝑓 climbs 3 units whenever π‘₯ increases by 2. The simplest choice for 𝑓 is a linear function of slope 3βˆ•2, for example 𝑓 (π‘₯) = 1.5π‘₯, so 𝑔(π‘₯) = 1.5π‘₯ + 3. 88. True. Using properties of exponents we see that:

( )π‘₯ π‘₯ 𝑓 (𝑔(π‘₯)) = 𝑓 (3π‘₯ ) = 23 = 23 = 8π‘₯ .

So, we see 𝑓 (𝑔(π‘₯)) = 8π‘₯ is exponential. Similarly, we can check 𝑔(𝑓 (π‘₯)) = 9π‘₯ is exponential. In general, the composition of two exponential functions of form 𝑦 = πΆπ‘Žπ‘₯ is exponential. 89. True. The graph of 𝑦 = 10π‘₯ is moved horizontally by β„Ž units if we replace π‘₯ by π‘₯βˆ’β„Ž for some number β„Ž. Writing 100 = 102 , we have 𝑓 (π‘₯) = 100(10π‘₯ ) = 102 β‹… 10π‘₯ = 10π‘₯+2 . The graph of 𝑓 (π‘₯) = 10π‘₯+2 is the graph of 𝑔(π‘₯) = 10π‘₯ shifted two units to the left. 90. True. If 𝑓 is increasing then its reflection about the line 𝑦 = π‘₯ is also increasing. An example is shown in Figure 1.38. The statement is true. 𝑦

π‘₯=𝑦

4 𝑓 (π‘₯)

βˆ’4

6

π‘₯

𝑓 βˆ’1 (π‘₯) βˆ’4

Figure 1.38 91. True. If 𝑓 (π‘₯) is even, we have 𝑓 (π‘₯) = 𝑓 (βˆ’π‘₯) for all π‘₯. For example, 𝑓 (βˆ’2) = 𝑓 (2). This means that the graph of 𝑓 (π‘₯) intersects the horizontal line 𝑦 = 𝑓 (2) at two points, π‘₯ = 2 and π‘₯ = βˆ’2. Thus, 𝑓 has no inverse function. 92. False. For example, 𝑓 (π‘₯) = π‘₯ and 𝑔(π‘₯) = π‘₯3 are both odd. Their inverses are 𝑓 βˆ’1 (π‘₯) = π‘₯ and 𝑔 βˆ’1 (π‘₯) = π‘₯1βˆ•3 . 2

93. False. For π‘₯ < 0, as π‘₯ increases, π‘₯2 decreases, so π‘’βˆ’π‘₯ increases. 94. True. We have 𝑔(βˆ’π‘₯) = 𝑔(π‘₯) since 𝑔 is even, and therefore 𝑓 (𝑔(βˆ’π‘₯)) = 𝑓 (𝑔(π‘₯)). 95. False. A counterexample is given by 𝑓 (π‘₯) = π‘₯2 and 𝑔(π‘₯) = π‘₯ + 1. The function 𝑓 (𝑔(π‘₯)) = (π‘₯ + 1)2 is not even because 𝑓 (𝑔(1)) = 4 and 𝑓 (𝑔(βˆ’1)) = 0 β‰  4. 96. True. The constant function 𝑓 (π‘₯) = 0 is the only function that is both even and odd. This follows, since if 𝑓 is both even and odd, then, for all π‘₯, 𝑓 (βˆ’π‘₯) = 𝑓 (π‘₯) (if 𝑓 is even) and 𝑓 (βˆ’π‘₯) = βˆ’π‘“ (π‘₯) (if 𝑓 is odd). Thus, for all π‘₯, 𝑓 (π‘₯) = βˆ’π‘“ (π‘₯) i.e. 𝑓 (π‘₯) = 0, for all π‘₯. So 𝑓 (π‘₯) = 0 is both even and odd and is the only such function. 97. True. A linear function can be written as 𝑦 = 𝑏 + π‘šπ‘₯. Hence, writing 𝑓 (π‘₯) = 𝑐 + 𝑛π‘₯ and 𝑔(π‘₯) = 𝑑 + 𝑝π‘₯ and using algebra, we see that: 𝑓 (𝑔(π‘₯)) = 𝑓 (𝑑 + 𝑝π‘₯) = 𝑐 + 𝑛(𝑑 + 𝑝π‘₯) = 𝑐 + 𝑛𝑑 + 𝑛𝑝π‘₯. So, setting 𝑏 = 𝑐 + 𝑛𝑑 and π‘š = 𝑛𝑝, we see that 𝑓 (𝑔(π‘₯)) is of the form 𝑏 + π‘šπ‘₯. Similarly, we can check 𝑔(𝑓 (π‘₯)) is of this form.


1.4 SOLUTIONS

37

98. Let 𝑓 (π‘₯) = π‘₯ and 𝑔(π‘₯) = βˆ’2π‘₯. Then 𝑓 (π‘₯) + 𝑔(π‘₯) = βˆ’π‘₯, which is decreasing. Note 𝑓 is increasing since it has positive slope, and 𝑔 is decreasing since it has negative slope. 99. This is impossible. If π‘Ž < 𝑏, then 𝑓 (π‘Ž) < 𝑓 (𝑏), since 𝑓 is increasing, and 𝑔(π‘Ž) > 𝑔(𝑏), since 𝑔 is decreasing, so βˆ’π‘”(π‘Ž) < βˆ’π‘”(𝑏). Therefore, if π‘Ž < 𝑏, then 𝑓 (π‘Ž) βˆ’ 𝑔(π‘Ž) < 𝑓 (𝑏) βˆ’ 𝑔(𝑏), which means that 𝑓 (π‘₯) + 𝑔(π‘₯) is increasing. 100. Let 𝑓 (π‘₯) = 𝑒π‘₯ and let 𝑔(π‘₯) = π‘’βˆ’2π‘₯ . Note 𝑓 is increasing since it is an exponential growth function, and 𝑔 is decreasing since it is an exponential decay function. Then 𝑓 (π‘₯)𝑔(π‘₯) = π‘’βˆ’π‘₯ , which is decreasing. 101. This is impossible. As π‘₯ increases, 𝑔(π‘₯) decreases. As 𝑔(π‘₯) decreases, so does 𝑓 (𝑔(π‘₯)) because 𝑓 is increasing (an increasing function increases as its variable increases, so it decreases as its variable decreases).

Solutions for Section 1.4 EXERCISES 1. Using the identity 𝑒ln π‘₯ = π‘₯, we have 𝑒ln(1βˆ•2) = 12 . 2. Using the identity 10log π‘₯ = π‘₯, we have

10log(𝐴𝐡) = 𝐴𝐡

3. Using the identity 𝑒ln π‘₯ = π‘₯, we have 5𝐴2 . 4. Using the identity ln (𝑒π‘₯ ) = π‘₯, we have 2AB. 5. Using the rules for ln, we have ln

( ) 1 + ln 𝐴𝐡 = ln 1 βˆ’ ln 𝑒 + ln 𝐴 + ln 𝐡 𝑒 = 0 βˆ’ 1 + ln 𝐴 + ln 𝐡 = βˆ’1 + ln 𝐴 + ln 𝐡.

6. Using the rules for ln, we have 2𝐴 + 3𝑒 ln 𝐡. 7. Taking logs of both sides log 3π‘₯ = π‘₯ log 3 = log 11 log 11 = 2.2. π‘₯= log 3 8. Taking logs of both sides log 17π‘₯ = log 2 π‘₯ log 17 = log 2 log 2 π‘₯= β‰ˆ 0.24. log 17 9. Isolating the exponential term 20 = 50(1.04)π‘₯ 20 = (1.04)π‘₯ . 50 Taking logs of both sides 2 = log(1.04)π‘₯ 5 2 log = π‘₯ log(1.04) 5 log(2βˆ•5) π‘₯= = βˆ’23.4. log(1.04)

log


38

Chapter One /SOLUTIONS

10. 5π‘₯ 4 = π‘₯ 7 3 ( )π‘₯ 4 5 = 7 3 Taking logs of both sides log

( ) ( ) 5 4 = π‘₯ log 7 3 log(4βˆ•7) π‘₯= β‰ˆ βˆ’1.1. log(5βˆ•3)

11. To solve for π‘₯, we first divide both sides by 5 and then take the natural logarithm of both sides. 7 = 𝑒0.2π‘₯ 5 ln(7βˆ•5) = 0.2π‘₯ ln(7βˆ•5) β‰ˆ 1.68. π‘₯= 0.2 12.

ln(2π‘₯ ) = ln(𝑒π‘₯+1 ) π‘₯ ln 2 = (π‘₯ + 1) ln 𝑒 π‘₯ ln 2 = π‘₯ + 1

0.693π‘₯ = π‘₯ + 1 1 π‘₯= β‰ˆ βˆ’3.26 0.693 βˆ’ 1 13. To solve for π‘₯, we first divide both sides by 600 and then take the natural logarithm of both sides. 50 = π‘’βˆ’0.4π‘₯ 600 ln(50βˆ•600) = βˆ’0.4π‘₯ ln(50βˆ•600) β‰ˆ 6.212. π‘₯= βˆ’0.4 14.

ln(2𝑒3π‘₯ ) = ln(4𝑒5π‘₯ ) ln 2 + ln(𝑒3π‘₯ ) = ln 4 + ln(𝑒5π‘₯ ) 0.693 + 3π‘₯ = 1.386 + 5π‘₯ π‘₯ = βˆ’0.347

15. Using the rules for ln, we get ln 7π‘₯+2 = ln 𝑒17π‘₯ (π‘₯ + 2) ln 7 = 17π‘₯ π‘₯(ln 7 βˆ’ 17) = βˆ’2 ln 7 βˆ’2 ln 7 β‰ˆ 0.26. π‘₯= ln 7 βˆ’ 17 16.

ln(10π‘₯+3 ) = ln(5𝑒7βˆ’π‘₯ ) (π‘₯ + 3) ln 10 = ln 5 + (7 βˆ’ π‘₯) ln 𝑒 2.303(π‘₯ + 3) = 1.609 + (7 βˆ’ π‘₯) 3.303π‘₯ = 1.609 + 7 βˆ’ 2.303(3) π‘₯ = 0.515


1.4 SOLUTIONS

39

17. Using the rules for ln, we have 2π‘₯ βˆ’ 1 = π‘₯2 2

π‘₯ βˆ’ 2π‘₯ + 1 = 0 (π‘₯ βˆ’ 1)2 = 0 π‘₯ = 1. 4𝑒2π‘₯βˆ’3 = 𝑒 + 5

18.

ln 4 + ln(𝑒2π‘₯βˆ’3 ) = ln(𝑒 + 5) 1.3863 + 2π‘₯ βˆ’ 3 = 2.0436 π‘₯ = 1.839. log π‘Ž 19. 𝑑 = . log 𝑏 ( ) log 𝑃𝑃 log 𝑃 βˆ’ log 𝑃0 0 = . 20. 𝑑 = log π‘Ž log π‘Ž 21. Taking logs of both sides yields 𝑛𝑑 = Hence 𝑑=

log

(

𝑄 𝑄0

ln 𝑃𝑃

0

π‘˜

.

=

log 𝑄 βˆ’ log 𝑄0 . 𝑛 log π‘Ž

( )𝑑 𝑄 π‘Ž = 0. 𝑏 𝑃0

𝑑=

𝑃 = π‘˜π‘‘, so 𝑑 = 24. ln 𝑃0

)

log π‘Ž

Hence

π‘Ž 23. 𝑑 = ln . 𝑏

𝑄 𝑄0

)

𝑛 log π‘Ž

22. Collecting similar terms yields

(

log

log

(

log

𝑄0

)

𝑃0

( ). π‘Ž 𝑏

.

25. Since we want (1.5)𝑑 = π‘’π‘˜π‘‘ = (π‘’π‘˜ )𝑑 , so 1.5 = π‘’π‘˜ , and π‘˜ = ln 1.5 = 0.4055. Thus, 𝑃 = 15𝑒0.4055𝑑 . Since 0.4055 is positive, this is exponential growth. 26. We want 1.7𝑑 = π‘’π‘˜π‘‘ so 1.7 = π‘’π‘˜ and π‘˜ = ln 1.7 = 0.5306. Thus 𝑃 = 10𝑒0.5306𝑑 . 27. We want 0.9𝑑 = π‘’π‘˜π‘‘ so 0.9 = π‘’π‘˜ and π‘˜ = ln 0.9 = βˆ’0.1054. Thus 𝑃 = 174π‘’βˆ’0.1054𝑑 . 28. Since we want (0.55)𝑑 = π‘’π‘˜π‘‘ = (π‘’π‘˜ )𝑑 , so 0.55 = π‘’π‘˜ , and π‘˜ = ln 0.55 = βˆ’0.5978. Thus 𝑃 = 4π‘’βˆ’0.5978𝑑 . Since βˆ’0.5978 is negative, this represents exponential decay. 29. If 𝑝(𝑑) = (1.04)𝑑 , then, for π‘βˆ’1 the inverse of 𝑝, we should have (1.04)𝑝

βˆ’1 (𝑑)

= 𝑑,

βˆ’1

𝑝 (𝑑) log(1.04) = log 𝑑, log 𝑑 β‰ˆ 58.708 log 𝑑. π‘βˆ’1 (𝑑) = log(1.04) 30. Since 𝑓 is increasing, 𝑓 has an inverse. To find the inverse of 𝑓 (𝑑) = 50𝑒0.1𝑑 , we replace 𝑑 with 𝑓 βˆ’1 (𝑑), and, since 𝑓 (𝑓 βˆ’1 (𝑑)) = 𝑑, we have βˆ’1 𝑑 = 50𝑒0.1𝑓 (𝑑) .


40

Chapter One /SOLUTIONS We then solve for 𝑓 βˆ’1 (𝑑): 𝑑 = 50𝑒0.1𝑓

βˆ’1 (𝑑)

βˆ’1 𝑑 = 𝑒0.1𝑓 (𝑑) 50 ( ) 𝑑 = 0.1𝑓 βˆ’1 (𝑑) ln 50 ( ) ( ) 1 𝑑 𝑑 = 10 ln . ln 𝑓 βˆ’1 (𝑑) = 0.1 50 50

31. Using 𝑓 (𝑓 βˆ’1 (𝑑)) = 𝑑, we see

𝑓 (𝑓 βˆ’1 (𝑑)) = 1 + ln 𝑓 βˆ’1 (𝑑) = 𝑑.

So ln 𝑓 βˆ’1 (𝑑) = 𝑑 βˆ’ 1 𝑓 βˆ’1 (𝑑) = π‘’π‘‘βˆ’1 .

PROBLEMS 32. Since 𝑦(0) = 𝐢𝑒0 = 𝐢 we have that 𝐢 = 2. Similarly, substituting π‘₯ = 1 gives 𝑦(1) = 2𝑒𝛼 so 2𝑒𝛼 = 1. Rearranging gives 𝑒𝛼 = 1βˆ•2. Taking logarithms we get 𝛼 = ln(1βˆ•2) = βˆ’ ln 2 = βˆ’0.693. Finally, 𝑦(2) = 2𝑒2(βˆ’ ln 2) = 2π‘’βˆ’2 ln 2 =

1 . 2

33. At the doubling time, 𝑑 = 10, we have 𝑝 = 2𝑝0 . Thus 𝑝0 𝑒10π‘˜ = 2𝑝0 𝑒10π‘˜ = 2 10π‘˜ = ln 2 1 ln 2 = 0.0693. π‘˜= 10 The function 𝑝 = 𝑝0 𝑒0.0693𝑑 has doubling time equal to 10. 34. At the doubling time, 𝑑 = 0.4, the we have 𝑝 = 2𝑝0 . Thus 𝑝0 𝑒0.4π‘˜ = 2𝑝0 𝑒0.4π‘˜ = 2 0.4π‘˜ = ln 2 1 ln 2 = 1.733. π‘˜= 0.4 The function 𝑝 = 𝑝0 𝑒1.733𝑑 has doubling time equal to 0.4. 35. Since ln 𝑓 (𝑑) = log𝑒 𝑓 (𝑑), we have Thus,

𝑒𝑓 (𝑑) = 𝑒ln 𝑑+2.3 = 𝑒ln 𝑑 β‹… 𝑒2.3 = 𝑑𝑒2.3 . 𝑓 (𝑑) = ln(𝑒𝑓 (𝑑) ) = ln(𝑑𝑒2.3 ).

Using the approximation 2.3 = ln 10 or 𝑒2.3 = 10, we have 𝑓 (𝑑) = ln(𝑑𝑒2.3 ) = ln(10𝑑).


1.4 SOLUTIONS

41

36. We can solve for the growth rate π‘˜ of the bacteria using the formula 𝑃 = 𝑃0 π‘’π‘˜π‘‘ : 1500 = 500π‘’π‘˜(2) ln(1500βˆ•500) π‘˜= . 2 Knowing the growth rate, we can find the population 𝑃 at time 𝑑 = 6: ln 3

𝑃 = 500𝑒( 2 )6 β‰ˆ 13,500 bacteria. 37. In ten years, the substance has decayed to 40% of its original mass. In another ten years, it will decay by an additional factor of 40%, so the amount remaining after 20 years will be 100 β‹… 40% β‹… 40% = 16 kg. 38. (a) Assuming the US population grows exponentially, we have population 𝑃 (𝑑) = 282.2π‘’π‘˜π‘‘ at time 𝑑 years after 2000. Using the 2018 population, which corresponds to 𝑑 = 18, we have 327.2 = 282.2𝑒18π‘˜ ln(327.2βˆ•282.2) π‘˜= = 0.0082198. 18 We want to find the time 𝑑 in which 350 = 282.2𝑒0.0082198𝑑 ln(350βˆ•282.2) 𝑑= = 26.195 years. 0.0082198 This model predicts the population to go over 350 million 26.195 years after 2000, in the year 2026. (b) Evaluate 𝑃 = 282.2𝑒0.0082198𝑑 for 𝑑 = 20 to find 𝑃 = 332.6 million people. 39. The population has increased by a factor of 48,000,000βˆ•40,000,000 = 1.2 in 10 years. Thus we have the formula 𝑃 = 40,000,000(1.2)π‘‘βˆ•10 , and π‘‘βˆ•10 gives the number of 10-year periods that have passed since 2005. In 2005, π‘‘βˆ•10 = 0, so we have 𝑃 = 40,000,000. In 2015, π‘‘βˆ•10 = 1, so 𝑃 = 40,000,000(1.2) = 48,000,000. In 2020, π‘‘βˆ•10 = 1.5, so 𝑃 = 40,000,000(1.2)1.5 β‰ˆ 52,581,000. To find the doubling time, solve 80,000,000 = 40,000,000(1.2)π‘‘βˆ•10 , to get 𝑑 = 38.02 years. 40. Let 𝑓 (𝑑) be oil consumption 𝑑 years after 2015. Since consumption is exponential, and 𝑓 (0) = 11.986 million barrels per day, we have 𝑓 (𝑑) = 11.986π‘’π‘˜π‘‘ . In 2018, when 𝑑 = 3, consumption was 13.525, so 𝑓 (3) = 13.525 11.986𝑒3𝑑 = 13.525 ) ( 13.525 3𝑑 = ln 11.986 π‘˜ = 0.040267. Our model predicts Chinese oil consumption in 2025, when 𝑑 = 10, to be 𝑓 (10) = 11.986𝑒0.040267(10) = 17.929 million barrels per day. 41. If 𝐢0 is the concentration of NO2 on the road, then the concentration π‘₯ meters from the road is 𝐢 = 𝐢0 π‘’βˆ’0.0254π‘₯ . We want to find the value of π‘₯ making 𝐢 = 𝐢0 βˆ•2, that is, 𝐢0 π‘’βˆ’0.0254π‘₯ =

𝐢0 . 2


42

Chapter One /SOLUTIONS Dividing by 𝐢0 and then taking natural logs yields ( ) ( ) 1 = βˆ’0.6931, ln π‘’βˆ’0.0254π‘₯ = βˆ’0.0254π‘₯ = ln 2 so π‘₯ = 27 meters. At 27 meters from the road the concentration of NO2 in the air is half the concentration on the road.

42. (a) Since the percent increase in deaths during a year is constant for constant increase in pollution, the number of deaths per year is an exponential function of the quantity of pollution. If 𝑄0 is the number of deaths per year without pollution, then the number of deaths per year, 𝑄, when the quantity of pollution is π‘₯ micrograms per cubic meter of air is 𝑄 = 𝑄0 (1.0033)π‘₯ . (b) We want to find the value of π‘₯ making 𝑄 = 2𝑄0 , that is, 𝑄0 (1.0033)π‘₯ = 2𝑄0 . Dividing by 𝑄0 and then taking natural logs yields ln ((1.0033)π‘₯ ) = π‘₯ ln 1.0033 = ln 2, so

ln 2 = 210.391. ln 1.0033 When there are 210.391 micrograms of pollutants per cubic meter of air, respiratory deaths per year are double what they would be in the absence of air pollution. π‘₯=

43. (a) From the table, we can see that the number of E85 vehicles increased by 393,553βˆ’302,341 = 91,212 between 2012 to 2017. Thus the percent increase is 91,212βˆ•302,341 = 0.302 = 30.2%. Alternatively, we see that 393,553βˆ•30,2341 = 1.302, again showing an increase of 30.2%. (b) To find 𝐴, we solve when 𝑑 = 0: π΄π‘’π‘Ÿβ‹…0 = 302,341 𝐴 β‹… 1 = 302,341 𝐴 = 302,341. Since 𝑑 is the number of years since 2012, we know that 𝑑 = 5 in 2017 and get: 393,553 = 302,341𝑒5π‘Ÿ . Solving for π‘Ÿ, we get 393,553 = 𝑒5π‘Ÿ 302,341 ( ) 393,553 ln = 5π‘Ÿ 302,341 π‘Ÿ = 0.052732. Substituting 𝑑 = 1, 2, 3, 4 into

302,341𝑒(0.052732)𝑑 ,

we find the remaining table values: Year

2012

2013

2014

2015

2016

2017

E85 vehicles

302,341

318,712

335,969

354,161

373,338

393,553

(c) The year 2011 is the year 𝑑 = βˆ’1. Therefore, If 𝑁 is the number of E85-powered vehicles in 2011, we have 𝑁 = 302,341𝑒0.052732(βˆ’1) = 286,811.


1.4 SOLUTIONS

43

44. (a) Since the initial amount of caffeine is 100 mg and the exponential decay rate is βˆ’0.17, we have 𝐴 = 100π‘’βˆ’0.17𝑑 . (b) See Figure 1.39. We estimate the half-life by estimating 𝑑 when the caffeine is reduced by half (so 𝐴 = 50); this occurs at approximately 𝑑 = 4 hours. 𝐴 (mg) 100

50

𝑑 (hours)

4

Figure 1.39 (c) We want to find the value of 𝑑 when 𝐴 = 50: 50 = 100π‘’βˆ’0.17𝑑 0.5 = π‘’βˆ’0.17𝑑 ln 0.5 = βˆ’0.17𝑑 𝑑 = 4.077. The half-life of caffeine is about 4.077 hours. This agrees with what we saw in Figure 1.39. 45. (a) The concentration decreases from 100 to 50 during the time from 1970 to 1975, a period of 5 years. (b) The concentration decreases from 50 to 25 during the time from 1975 to 1980, a period of 5 years. (c) The decay is exponential if the half-life of the concentration is the same beginning at any concentration level. We only checked at two levels, 100 and 50, but for those the half-lives were both 5 years. This is some evidence that the decay might be exponential. Also, if we look at any other 5-year period, we can check that the concentration appears to decreases by half. (d) Since the initial value of concentration is 100, an exponential model is of the form 𝐢 = 100π‘’π‘˜π‘‘ . We can evaluate π‘˜ by using the value 𝐢 = 25 at 𝑑 = 10. 25 = 100𝑒10π‘˜ 0.25 = 𝑒10π‘˜ ln(0.25) = 10π‘˜ π‘˜ = βˆ’0.139. An exponential model is given by

𝐢 = 100π‘’βˆ’0.139𝑑 .

Alternative solution. Using the half-life 𝑇 = 5 years, we have 𝐢 = 100 β‹… 2βˆ’π‘‘βˆ•π‘‡ = 100 β‹… 2βˆ’π‘‘βˆ•5 . 46. (a) The initial dose is 10 mg. (b) Since 0.82 = 1 βˆ’ 0.18, the decay rate is 0.18, so 18% leaves the body each hour. (c) When 𝑑 = 6, we have 𝐴 = 10(0.82)6 = 3.04. The amount in the body after 6 hours is 3.04 mg. (d) We want to find the value of 𝑑 when 𝐴 = 1. Using logarithms: 1 = 10(0.82)𝑑 0.1 = (0.82)𝑑 ln(0.1) = 𝑑 ln(0.82) 𝑑 = 11.60 hours. After 11.60 hours, the amount is 1 mg.


44

Chapter One /SOLUTIONS

47. (a) Since there is a 4% increase per degree Fahrenheit, at temperature 𝑇 β—¦ F, we have 𝑄 = 𝑄0 (1.04)𝑇 βˆ’32 . (b) At 50β—¦ F, we have

𝑄1 = 𝑄0 (1.04)50βˆ’32 = 𝑄0 (1.04)18 .

β—¦

And at 14 F, we have Thus

𝑄2 = 𝑄0 (1.04)14βˆ’32 = 𝑄0 (1.04)βˆ’18 . 𝑄 (1.04)βˆ’18 𝑄2 = 0 = 1.04βˆ’36 = 0.244. 𝑄1 𝑄0 (1.04)18

So the quantity of water in the air at 14β—¦ F is about 24% of the quantity at 50β—¦ F. (c) The temperature rise that doubles the quantity of moisture that can be absorbed is given by 2𝑄0 = 𝑄0 (1.04)𝑇 (1.04)𝑇 = 2 𝑇 ln 1.04 = ln 2 ln 2 = 17.7. 𝑇 = ln 1.04 So an approximately 18β—¦ F temperature rise doubles the amount of moisture that can be absorbed. 48. To find a half-life, we want to find at what 𝑑 value 𝑄 = 12 𝑄0 . Plugging this into the equation of the decay of plutonium-240, we have 1 = π‘’βˆ’0.00011𝑑 2 ln(1βˆ•2) 𝑑= β‰ˆ 6,301 years. βˆ’0.00011 The only difference in the case of plutonium-242 is that the constant βˆ’0.00011 in the exponent is now βˆ’0.0000018. Thus, following the same procedure, the solution for 𝑑 is 𝑑=

ln(1βˆ•2) β‰ˆ 385,081 years. βˆ’0.0000018

49. Given the doubling time of 5 hours, we can solve for the bacteria’s growth rate; 2𝑃0 = 𝑃0 π‘’π‘˜5 ln 2 π‘˜= . 5 So the growth of the bacteria population is given by: 𝑃 = 𝑃0 𝑒ln(2)π‘‘βˆ•5 . We want to find 𝑑 such that

3𝑃0 = 𝑃0 𝑒ln(2)π‘‘βˆ•5 .

Therefore we divide both sides by 𝑃0 and apply ln. We get 𝑑=

5 ln(3) = 7.925 hours. ln(2)

50. (a) The pressure 𝑃 at 6194 meters is given in terms of the pressure 𝑃0 at sea level to be 𝑃 = 𝑃0 π‘’βˆ’0.00012β„Ž = 𝑃0 𝑒(βˆ’0.00012)6194 = 𝑃0 π‘’βˆ’0.74328 β‰ˆ 0.4756𝑃0

or about 47.6% of sea level pressure.


1.4 SOLUTIONS

45

(b) At β„Ž = 12,000 meters, we have 𝑃 = 𝑃0 π‘’βˆ’0.00012β„Ž = 𝑃0 𝑒(βˆ’0.00012)12,000 = 𝑃0 π‘’βˆ’1.44 β‰ˆ 0.2369𝑃0

or about 23.7% of sea level pressure.

51. (a) 𝐡(𝑑) = 𝐡0 𝑒0.067𝑑 (b) 𝑃 (𝑑) = 𝑃0 𝑒0.033𝑑 (c) If the initial price is $50, then

𝐡(𝑑) = 50𝑒0.067𝑑 𝑃 (𝑑) = 50𝑒0.033𝑑 .

We want the value of 𝑑 such that

𝐡(𝑑) = 2𝑃 (𝑑) 50𝑒0.067𝑑 = 2 β‹… 50𝑒0.033𝑑 𝑒0.067𝑑 = 𝑒0.034𝑑 = 2 𝑒0.033𝑑 ln 2 𝑑= = 20.387 years . 0.034 Thus, when 𝑑 = 20.387 the price of the textbook was predicted to be double what it would have been had the price risen by inflation only. This occurred in the year 2000.

52. (a) We assume 𝑓 (𝑑) = π΄π‘’βˆ’π‘˜π‘‘ , where 𝐴 is the initial population, so 𝐴 = 100,000. When 𝑑 = 110, there were 3200 tigers, so 3200 = 100,000π‘’βˆ’π‘˜β‹…110 Solving for π‘˜ gives 3200 = 0.032 π‘’βˆ’π‘˜β‹…110 = 100,000 1 π‘˜=βˆ’ ln(0.032) = 0.0313 = 3.13% 110 so 𝑓 (𝑑) = 100,000π‘’βˆ’0.0313𝑑 . (b) In 2000, the predicted number of tigers was 𝑓 (100) = 100,000π‘’βˆ’0.0313(100) = 4372. In 2010, we know the number of tigers was 3200. The predicted percent reduction is 3200 βˆ’ 4372 = βˆ’0.268 = βˆ’26.8%. 4372 Thus the actual decrease is larger than the predicted decrease. 53. The population of China, 𝐢, in billions, is given by 𝐢 = 1.379(1.0041)𝑑 where 𝑑 is time in years from 2017, and the population of India, 𝐼, in billions, is given by 𝐼 = 1.282(1.0117)𝑑 . The two populations will be equal when 𝐢 = 𝐼, thus, we must solve the equation: 1.379(1.0041)𝑑 = 1.282(1.0117)𝑑 for 𝑑, which leads to

(1.0117)𝑑 ( 1.0117 )𝑑 1.379 = . = 1.282 (1.0041)𝑑 1.0041

Taking logs on both sides, we get 𝑑 log so

1.0117 1.379 = log , 1.0041 1.282

log (1.379βˆ•1.282) = 9.67 years. log (1.0117βˆ•1.0041) This model predicts the population of India will exceed that of China in 2026. 𝑑=


46

Chapter One /SOLUTIONS

54. Let 𝐴 represent the revenue (in billions of dollars) at Apple 𝑑 years since 2013. Since 𝐴 = 54.5 when 𝑑 = 0 and we want the continuous growth rate, we write 𝐴 = 54.5π‘’π‘˜π‘‘ . We use the information from 2015, that 𝐴 = 74.6 when 𝑑 = 2, to find π‘˜: 74.6 = 54.5π‘’π‘˜β‹…2 1.37 = 𝑒2π‘˜ ln(1.37) = 2π‘˜ π‘˜ = 0.157. We have 𝐴 = 54.5𝑒0.157𝑑 , which represents a continuous growth rate of 15.7% per year. 55. Let 𝑃 (𝑑) be the world population in billions 𝑑 years after 2010. (a) Assuming exponential growth, we have

𝑃 (𝑑) = 6.9π‘’π‘˜π‘‘ .

In 2050, we have 𝑑 = 40 and we expect the population then to be 9 billion, so 9 = 6.9π‘’π‘˜β‹…40 . Solving for π‘˜, we have π‘’π‘˜β‹…40 =

9 6.9

) ( 1 9 = 0.00664 = 0.664% per year. ln 40 6.9 (b) The β€œDay of 8 Billion” should occur when 8 = 6.9𝑒0.00664𝑑 . π‘˜=

Solving for 𝑑 gives 8 6.9 ln(8βˆ•6.9) 𝑑= = 22.277 years. 0.00664

𝑒0.00664𝑑 =

So the β€œDay of 8 Billion” should be 22.277 years after the end of 2010. This is 22 years and 0.277 β‹… 365 β‰ˆ 101 days; so 101 days into 2032. That is, April 11, 2032. This solution does not take leap years into account. 56. If π‘Ÿ was the average yearly inflation rate, in decimals, then 14 (1 + π‘Ÿ)3 = 2,400,000, so π‘Ÿ = 211.53, i.e. π‘Ÿ = 21,153%. 57. If 𝑑 is time in decades, then the number of vehicles, 𝑉 , in millions, is given by 𝑉 = 246(1.155)𝑑 . For time 𝑑 in decades, the number of people, 𝑃 , in millions, is given by 𝑃 = 308.7(1.097)𝑑 . There is an average of one vehicle per person when

𝑉 = 1, or 𝑉 = 𝑃 . Thus, we solve for 𝑑 in the equation: 𝑃

246(1.155)𝑑 = 308.7(1.097)𝑑 , which leads to

(

1.155 1.097

Taking logs on both sides, we get 𝑑 log so

)𝑑

=

(1.155)𝑑 308.7 = (1.097)𝑑 246

308.7 1.155 = log , 1.097 246

log (308.7βˆ•246) = 4.41 decades. log (1.155βˆ•1.097) This model predicts one vehicle per person in 2054. 𝑑=


1.4 SOLUTIONS

47

58. For an exponentially growing population, 𝑝 = 𝑝0 π‘’π‘˜π‘‘ , that doubles in 𝑛 days, we find the continuous growth rate π‘˜ in terms of 𝑛. Since 𝑝 = 2𝑝0 when 𝑑 = 𝑛, we have 2𝑝0 = 𝑝0 π‘’π‘˜π‘› π‘’π‘˜π‘› = 2 π‘˜π‘› = ln 2 1 π‘˜ = ln 2 𝑛 𝑝 = 𝑝0 𝑒(ln 2)π‘‘βˆ•π‘› . Doubling time for the phytoplankton population, 𝑃 , is 0.5 days, and for the foraminifera population, 𝐹 , it is 5 days. If they both initially have the same population 𝐢, then after 𝑑 days we have 𝑃 = 𝐢𝑒(ln 2)π‘‘βˆ•0.5 = 𝐢𝑒1.3863𝑑 𝐹 = 𝐢𝑒(ln 2)π‘‘βˆ•5 = 𝐢𝑒0.13863𝑑 . (a) We have 𝑃 = 2𝐹 𝐢𝑒1.3863𝑑 = 2𝐢𝑒0.13863𝑑 𝑒1.3863𝑑 = 2𝑒0.13863𝑑 1.3863𝑑 = ln 2 + 0.13863𝑑 1.24767𝑑 = ln 2 𝑑 = 0.556 days. The phytoplankton population is double the foraminifera population after 0.556 days, a little over 13 hours. (b) We have 𝑃 = 1000𝐹 𝐢𝑒

1.3863𝑑

= 1000𝐢𝑒0.13863𝑑

𝑒1.3863𝑑 = 1000𝑒0.13863𝑑 1.3863𝑑 = ln 1000 + 0.13863𝑑 1.24767𝑑 = ln 1000 𝑑 = 5.537 days. The phytoplankton population is 1000 times the foraminifera population after 5.537 days, about five and a half days. 59. We assume exponential decay and solve for π‘˜ using the half-life: π‘’βˆ’π‘˜(5730) = 0.5

so

π‘˜ = 1.21 β‹… 10βˆ’4 .

= 0.995,

𝑑=

ln 0.995 = 41.43 years. βˆ’1.21 β‹… 10βˆ’4

Now find 𝑑, the age of the painting: βˆ’4 𝑑

π‘’βˆ’1.21β‹…10

so

Since Vermeer died in 1675, the painting is a fake. 60. (a) We find an exponential model in the form 𝑐(𝑑) = 𝑐0 π‘Žπ‘‘ . Using 𝑐(0) = 25 and 𝑐(1) = 21.8, we have 𝑐(𝑑) = 25π‘Žπ‘‘ 21.8 = 25π‘Ž1 = 25π‘Ž. Thus

21.8 = 0.872 25 𝑐(𝑑) = 25(0.872)𝑑 .

π‘Ž=

Alternately, we could use 𝑐(𝑑) = 𝑐0 π‘’π‘˜π‘‘ . Then we have 21.8 = 25π‘’π‘˜β‹…1 = 25π‘’π‘˜ , giving ) ( 21.8 = ln(0.872) = βˆ’0.136966 π‘˜ = ln 25 𝑐(𝑑) = 25π‘’βˆ’0.136966𝑑 .


48

Chapter One /SOLUTIONS (b) We find 𝑑 so that 25(0.872)𝑑 = 10, giving 10 25 ( ) 10 𝑑 ln(0.872) = ln 25 ln(10βˆ•25) 𝑑= = 6.6899. ln(0.872) (0.872)𝑑 =

Alternatively, solving 25π‘’βˆ’0.136966𝑑 = 10 gives ln(10βˆ•25) = 6.6899. 0.136966 Using either method shows that it takes 6.690 years for the cyanide concentration to fall to 10 ppm. (c) If 𝐷(𝑑) = 𝑐(2𝑑), then ( )𝑑 𝐷(𝑑) = 25(0.872)2𝑑 = 25 0.8722 = 25(0.7604)𝑑 . 𝑑=βˆ’

Alternatively,

𝐷(𝑑) = 25π‘’βˆ’0.136966(2𝑑) = 25π‘’βˆ’0.273932𝑑 .

(d) Starting three years earlier, but with 𝑑 measured from the original time, we have 𝐸(𝑑) = 𝑐(𝑑 + 3), so 𝐸(𝑑) = 25(0.872)𝑑+3 = 25(0.872)3 (0.872)𝑑 = 16.576(0.872)𝑑 . Alternatively,

𝐸(𝑑) = 25π‘’βˆ’0.136966(𝑑+3) = 25π‘’βˆ’0.136966(3) π‘’βˆ’0.136966𝑑 = 16.576π‘’βˆ’0.136966𝑑 .

61. Let π‘Š1 be the strength of the first earthquake and let π‘Š2 be the strength of the second earthquake. Then ( ) π‘Š1 𝑅1 = log = 7.8 π‘Š0 ( ) π‘Š2 = 7.3. 𝑅2 = log π‘Š0 (a) We want to know π‘Š1 βˆ•π‘Š0 , so we raise the expression for 𝑅1 to the tenth power: π‘Š1 = 107.8 = 63,095,734 β‰ˆ 63 million. π‘Š0 (b) We want to know π‘Š1 βˆ•π‘Š2 , so we subtract the two expressions for 𝑅1 and 𝑅2 , giving ( ) ( ) ( ) ( ) π‘Š1 βˆ•π‘Š0 π‘Š1 π‘Š2 π‘Š1 βˆ’ log = log = log = 7.8 βˆ’ 7.3 = 0.5. 𝑅1 βˆ’ 𝑅2 = log π‘Š0 π‘Š0 π‘Š2 βˆ•π‘Š0 π‘Š2 To find the ratio π‘Š1 βˆ•π‘Š1 we raise to the tenth power: π‘Š1 = 100.5 = 3.162. π‘Š2 The first earthquake was just over three times as large as the second one. 62. We know that the 𝑦-intercept of the line is at (0,1), so we need one other point to determine the equation of the line. We observe that it intersects the graph of 𝑓 (π‘₯) = 10π‘₯ at the point π‘₯ = log 2. The 𝑦-coordinate of this point is then 𝑦 = 10π‘₯ = 10log 2 = 2, so (log 2, 2) is the point of intersection. We can now find the slope of the line: π‘š=

2βˆ’1 1 = . log 2 βˆ’ 0 log 2

Plugging this into the point-slope formula for a line, we have 𝑦 βˆ’ 𝑦1 = π‘š(π‘₯ βˆ’ π‘₯1 ) 1 (π‘₯ βˆ’ 0) π‘¦βˆ’1 = log 2 1 𝑦= π‘₯ + 1 β‰ˆ 3.3219π‘₯ + 1. log 2


1.4 SOLUTIONS

49

63. (a) Since 𝑒0 = 1 and 100 = 1, we know that log𝑒 1 = 0 and log10 1 = 0. Thus the π‘₯-intercept is π‘₯ = 1. (b) Looking at values of π‘₯ > 1, say π‘₯ = 2, we have log𝑒 2 β‰ˆ 0.7 (because 𝑒0.7 β‰ˆ 2) and log10 2 β‰ˆ 0.3 (because 100.3 β‰ˆ 2), so A is log𝑒 π‘₯ and B is log10 π‘₯. For 0 < π‘₯ < 1, say π‘₯ = 0.5, we have log𝑒 0.5 β‰ˆ βˆ’0.7 and log10 0.5 β‰ˆ βˆ’0.3, so C is log10 π‘₯ and D is log𝑒 π‘₯. 64. The function 𝑒π‘₯ has a vertical intercept of 1, so must be 𝐴. The function ln π‘₯ has an π‘₯-intercept of 1, so must be 𝐷. The graphs of π‘₯2 and π‘₯1βˆ•2 go through the origin. The graph of π‘₯1βˆ•2 is concave down so it corresponds to graph 𝐢 and the graph of π‘₯2 is concave up so it corresponds to graph 𝐡. 65. Since 𝑄 = 𝑄0 π‘’π‘˜π‘‘ , the doubling time, 𝑇 , is given by 2𝑄0 = 𝑄0 π‘’π‘˜π‘‡ ln 2 𝑇 = . π‘˜ Thus, doubling π‘˜ does not double 𝑇 ; it halves it. 66. Yes, ln(ln(π‘₯)) means take the ln of the value of the function ln π‘₯. On the other hand, ln2 (π‘₯) means take the function ln π‘₯ and square it. For example, consider each of these functions evaluated at 𝑒. Since ln 𝑒 = 1, ln2 𝑒 = 12 = 1, but ln(ln(𝑒)) = ln(1) = 0. See the graphs in Figure 1.40. (Note that ln(ln(π‘₯)) is only defined for π‘₯ > 1.)

2 1 βˆ’1

1

𝑓 (π‘₯) = ln π‘₯ 1

2

3

4

5

βˆ’1 βˆ’2

2

𝑓 (π‘₯) = ln(ln π‘₯) 1

2

3

1 4

𝑓 (π‘₯) = ln2 π‘₯

5 1

2

3

4

5

Figure 1.40 67. (a) The 𝑦-intercept of β„Ž(π‘₯) = ln(π‘₯ + π‘Ž) is β„Ž(0) = ln π‘Ž. Thus increasing π‘Ž increases the 𝑦-intercept. (b) The π‘₯-intercept of β„Ž(π‘₯) = ln(π‘₯ + π‘Ž) is where β„Ž(π‘₯) = 0. Since this occurs where π‘₯ + π‘Ž = 1, or π‘₯ = 1 βˆ’ π‘Ž, increasing π‘Ž moves the π‘₯-intercept to the left. 68. The vertical asymptote is where π‘₯ + π‘Ž = 0, or π‘₯ = βˆ’π‘Ž. Thus increasing π‘Ž moves the vertical asymptote to the left. 69. (a) The 𝑦-intercept of 𝑔(π‘₯) = ln(π‘Žπ‘₯ + 2) is 𝑔(0) = ln 2. Thus increasing π‘Ž does not effect the 𝑦-intercept. (b) The π‘₯-intercept of 𝑔(π‘₯) = ln(π‘Žπ‘₯ + 2) is where 𝑔(π‘₯) = 0. Since this occurs where π‘Žπ‘₯ + 2 = 1, or π‘₯ = βˆ’1βˆ•π‘Ž, increasing π‘Ž moves the π‘₯-intercept toward the origin. (The intercept is to the left of the origin if π‘Ž > 0 and to the right if π‘Ž < 0.) 70. The vertical asymptote is where π‘₯ + 2 = 0, or π‘₯ = βˆ’2, so increasing π‘Ž does not effect the vertical asymptote. 71. The vertical asymptote is where π‘Žπ‘₯ + 2 = 0, or π‘₯ = βˆ’2βˆ•π‘Ž. Thus increasing π‘Ž moves the vertical asymptote toward the origin. (The asymptote is to the left of the origin for π‘Ž > 0 and to the right of the origin for π‘Ž < 0.) 72. Properties of logs give

ln(𝑃0 π‘’π‘˜π‘‘ ) = ln 𝑃0 + ln π‘’π‘˜π‘‘ = ln 𝑃0 + π‘˜π‘‘.

Therefore ln(𝑃0 π‘’π‘˜π‘‘2 ) βˆ’ ln(𝑃0 π‘’π‘˜π‘‘1 ) ln 𝑓 (𝑑2 ) βˆ’ ln 𝑓 (𝑑1 ) = 𝑑2 βˆ’ 𝑑1 𝑑2 βˆ’ 𝑑1 ln 𝑃0 + π‘˜π‘‘2 βˆ’ ln 𝑃0 βˆ’ π‘˜π‘‘1 = 𝑑2 βˆ’ 𝑑1 π‘˜(𝑑2 βˆ’ 𝑑1 ) = = π‘˜. 𝑑2 βˆ’ 𝑑1

Strengthen Your Understanding 73. The function βˆ’ log |π‘₯| is even, since | βˆ’ π‘₯| = |π‘₯|, which means βˆ’ log | βˆ’ π‘₯| = βˆ’ log |π‘₯|.


50

Chapter One /SOLUTIONS

74. We have

ln(100π‘₯) = ln(100) + ln π‘₯.

In general, ln(100π‘₯) β‰  100 β‹… ln π‘₯. 75. As seen from the graphs of the functions, this inequality holds only for π‘₯ > 1. The functions cross at the point (1, 0) and the inequality is reversed for π‘₯ < 1. 76. The correct property says that the logarithm of a product is the sum of the logarithms, that is ln(𝐴𝐡) = ln 𝐴 + ln 𝐡. We may also check that the given property is not correct by taking 𝐴 = 𝐡 = 1. Then the statement gives us the incorrect statement: ln 2 = 2 ln 1 = 0. 77. One of the properties of logarithms states that the logarithm of a product is the sum of the logarithms, that is ln(𝐴𝐡) = ln 𝐴 + ln 𝐡. There is no property of logarithms that states the logarithm of a sum is the sum of logarithms. We can check by taking 𝐴 = 𝐡 = 1. Then the statement gives us the incorrect statement: ln 2 = ln 1 + ln 1 = 0. 78. The functions 𝑦 = ln π‘₯ and 𝑦 = 𝑒π‘₯ are inverses of each other, but not reciprocals of each other. As their graphs show, 𝑦 = 1βˆ• ln π‘₯ and 𝑦 = 𝑒π‘₯ don’t even have the same domain. 79. The function 𝑦 = 0.7 log π‘₯ works, as it scales down each value of 𝑦 = log π‘₯ for π‘₯ > 1. The graph of 𝑦 = 0.7 log π‘₯ is below the graph of 𝑦 = log π‘₯ as long as π‘₯ > 1. 80. One possibility is 𝑓 (π‘₯) = βˆ’π‘₯, because ln(βˆ’π‘₯) is only defined if βˆ’π‘₯ > 0. 81. One possibility is 𝑓 (π‘₯) = ln(π‘₯ βˆ’ 3). 82. True, as seen from the graph. 83. False, since log(π‘₯ βˆ’ 1) = 0 if π‘₯ βˆ’ 1 = 1, so π‘₯ = 2. 84. False. The inverse function is 𝑦 = 10π‘₯ . 85. False, since π‘Žπ‘₯ + 𝑏 = 0 if π‘₯ = βˆ’π‘βˆ•π‘Ž. Thus 𝑦 = ln(π‘Žπ‘₯ + 𝑏) has a vertical asymptote at π‘₯ = βˆ’π‘βˆ•π‘Ž.

Solutions for Section 1.5 EXERCISES 1. See Figure 1.41.

) 3πœ‹ = βˆ’1 is negative. 2 ( ) 3πœ‹ cos =0 2 ( ) 3πœ‹ tan is undefined. 2 sin

(

-

Figure 1.41


1.5 SOLUTIONS 2. See Figure 1.42. sin(2πœ‹) = 0 cos(2πœ‹) = 1 is positive. tan(2πœ‹) = 0

6

Figure 1.42 3. See Figure 1.43. πœ‹ 4 πœ‹ cos 4 πœ‹ tan 4 sin

is positive is positive is positive

I

Figure 1.43 4. See Figure 1.44. sin 3πœ‹ = 0 cos 3πœ‹ = βˆ’1 is negative tan 3πœ‹ = 0

?

Figure 1.44

51


52

Chapter One /SOLUTIONS 5. See Figure 1.45.

( ) πœ‹ is positive. 6 ( ) πœ‹ cos is positive. 6 ( ) πœ‹ tan is positive. 6 sin

M

Figure 1.45 6. See Figure 1.46. 4πœ‹ 3 4πœ‹ cos 3 4πœ‹ tan 3 sin

is negative is negative is positive

j

Figure 1.46 7. See Figure 1.47.

) βˆ’4πœ‹ is positive. 3 ) ( βˆ’4πœ‹ is negative. cos 3 ) ( βˆ’4πœ‹ is negative. tan 3 sin

(

*

Figure 1.47


1.5 SOLUTIONS 8. 4 radians β‹…

180β—¦ = πœ‹ radians

(

720 πœ‹

)β—¦

53

β‰ˆ 240β—¦ . See Figure 1.48. sin 4

is negative

cos 4

is negative

tan 4

is positive.

j

Figure 1.48 9. βˆ’1 radian β‹…

180β—¦

πœ‹ radians

=βˆ’

(

180β—¦ πœ‹

)

β‰ˆ βˆ’60β—¦ . See Figure 1.49. sin (βˆ’1)

is negative

cos (βˆ’1)

is positive

tan (βˆ’1)

is negative.

Figure 1.49 10. The period is 2πœ‹βˆ•3, because when 𝑑 varies from 0 to 2πœ‹βˆ•3, the quantity 3𝑑 varies from 0 to 2πœ‹. The amplitude is 7, since the value of the function oscillates between βˆ’7 and 7. 11. The period is 2πœ‹βˆ•(1βˆ•4) = 8πœ‹, because when 𝑒 varies from 0 to 8πœ‹, the quantity π‘’βˆ•4 varies from 0 to 2πœ‹. The amplitude is 3, since the function oscillates between 2 and 8. 12. The period is 2πœ‹βˆ•2 = πœ‹, because as π‘₯ varies from βˆ’πœ‹βˆ•2 to πœ‹βˆ•2, the quantity 2π‘₯ + πœ‹ varies from 0 to 2πœ‹. The amplitude is 4, since the function oscillates between 4 and 12. 13. The period is 2πœ‹βˆ•πœ‹ = 2, since when 𝑑 increases from 0 to 2, the value of πœ‹π‘‘ increases from 0 to 2πœ‹. The amplitude is 0.1, since the function oscillates between 1.9 and 2.1. ( ) π‘₯ . 14. This graph is a sine curve with period 8πœ‹ and amplitude 2, so it is given by 𝑓 (π‘₯) = 2 sin 4 ( ) π‘₯ . 15. This graph is a cosine curve with period 6πœ‹ and amplitude 5, so it is given by 𝑓 (π‘₯) = 5 cos 3 16. This graph is an inverted sine curve with amplitude 4 and period πœ‹, so it is given by 𝑓 (π‘₯) = βˆ’4 sin(2π‘₯). ( ) π‘₯ . 17. This graph is an inverted cosine curve with amplitude 8 and period 20πœ‹, so it is given by 𝑓 (π‘₯) = βˆ’8 cos 10 18. This graph has period 6, amplitude 5 and no vertical or horizontal shift, so it is given by ( ) ( ) 2πœ‹ πœ‹ 𝑓 (π‘₯) = 5 sin π‘₯ = 5 sin π‘₯ . 6 3 19. The graph is a cosine curve with period 2πœ‹βˆ•5 and amplitude 2, so it is given by 𝑓 (π‘₯) = 2 cos(5π‘₯).


54

Chapter One /SOLUTIONS

20. The graph is an inverted sine curve with amplitude 1 and period 2πœ‹, shifted up by 2, so it is given by 𝑓 (π‘₯) = 2 βˆ’ sin π‘₯. 21. This can be represented by a sine function of amplitude 3 and period 18. Thus, ( ) πœ‹ π‘₯ . 𝑓 (π‘₯) = 3 sin 9 ( ) π‘₯ + 2. 4 23. This graph has period 8, amplitude 3, and a vertical shift of 3 with no horizontal shift. It is given by ) ( ) ( πœ‹ 2πœ‹ π‘₯ = 3 + 3 sin π‘₯ . 𝑓 (π‘₯) = 3 + 3 sin 8 4 22. This graph is the same as in Problem 14 but shifted up by 2, so it is given by 𝑓 (π‘₯) = 2 sin

24.

πœ‹ 5

M

) ( πœ‹ πœ‹ = cos cos βˆ’ (by picture) 5 5 = 0.809.

πœ‹ 5

25. (0,1) πœ‹ 5

1

sin πœ‹5 cos πœ‹5

sin πœ‹5

(1,0)

cos πœ‹5

By the Pythagorean Theorem, (cos πœ‹5 )2 + (sin πœ‹5 )2 = 12 ; √ √ so (sin πœ‹5 )2 = 1 βˆ’ (cos πœ‹5 )2 , and sin πœ‹5 = 1 βˆ’ (cos πœ‹5 )2 = 1 βˆ’ (0.809)2 β‰ˆ 0.588.

26.

We take the positive square root since by the picture we know that sin πœ‹5 is positive. (0,1)

πœ‹ sin 12

πœ‹ cos 12

πœ‹ cos 12 πœ‹ 12

(1,0)

√

πœ‹ sin 12

1

πœ‹ 2 πœ‹ 2 πœ‹ 2 πœ‹ 2 πœ‹ By the Pythagorean Theorem, (cos 12 ) + (sin 12 ) = 12 ; so (cos 12 ) = 1 βˆ’ (sin 12 ) and cos 12 =

√ πœ‹ 2 1 βˆ’ (sin 12 ) =

πœ‹ 1 βˆ’ (0.259)2 β‰ˆ 0.966. We take the positive square root since by the picture we know that cos 12 is positive.


1.5 SOLUTIONS ) ( ) ( πœ‹ πœ‹ = βˆ’ sin = βˆ’0.259. 27. Since sin πœƒ is an odd function, sin βˆ’ 12 12 πœ‹ first. We can use the Pythagorean identity sin2 πœƒ + cos2 πœƒ = 1 to find 28. Since tan πœƒ = sin πœƒβˆ• cos πœƒ, we need to find cos 12 √ πœ‹ cos = Β± 1 βˆ’ 0.2592 = Β±0.966. 12 πœ‹ Since the angle πœƒ = lies in the first quadrant, cos πœƒ = 0.966. Thus, 12 tan

πœ‹ 0.259 = = 0.268. 12 0.966

πœ‹ first. We can use the Pythagorean identity sin2 πœƒ + cos2 πœƒ = 1 to find 5 √ πœ‹ sin = Β± 1 βˆ’ 0.8092 = Β±0.588. 5

29. Since tan πœƒ = sin πœƒβˆ• cos πœƒ, we need to find sin

Since the angle πœƒ =

πœ‹ lies in the first quadrant, sin πœ‹5 = 0.588. Thus, 5 tan

0.588 πœ‹ = = 0.727. 5 0.809

30. We first divide by 5 and then use inverse sine: 2 = sin(3π‘₯) 5 βˆ’1 sin (2βˆ•5) = 3π‘₯ π‘₯=

sinβˆ’1 (2βˆ•5) β‰ˆ 0.1372. 3

There are infinitely many other possible solutions since the sine is periodic. 31. We first isolate cos(2π‘₯ + 1) and then use inverse cosine: 1 = 8 cos(2π‘₯ + 1) βˆ’ 3 4 = 8 cos(2π‘₯ + 1) 0.5 = cos(2π‘₯ + 1) cosβˆ’1 (0.5) = 2π‘₯ + 1 cosβˆ’1 (0.5) βˆ’ 1 π‘₯= β‰ˆ 0.0236. 2 There are infinitely many other possible solutions since the cosine is periodic. 32. We first isolate tan(5π‘₯) and then use inverse tangent: 8 = 4 tan(5π‘₯) 2 = tan(5π‘₯) tanβˆ’1 2 = 5π‘₯ tanβˆ’1 2 π‘₯= = 0.221. 5 There are infinitely many other possible solutions since the tangent is periodic. 33. We first isolate (2π‘₯ + 1) and then use inverse tangent: 1 = 8 tan(2π‘₯ + 1) βˆ’ 3 4 = 8 tan(2π‘₯ + 1) 0.5 = tan(2π‘₯ + 1) arctan(0.5) = 2π‘₯ + 1 arctan(0.5) βˆ’ 1 π‘₯= = βˆ’0.268. 2 There are infinitely many other possible solutions since the tangent is periodic.

55


56

Chapter One /SOLUTIONS

34. We first isolate sin(5π‘₯) and then use inverse sine: 8 = 4 sin(5π‘₯) 2 = sin(5π‘₯). But this equation has no solution since βˆ’1 ≀ sin(5π‘₯) ≀ 1. 35. The earth makes one revolution around the sun in one year, so its period is one year. 36. The moon makes one revolution around the earth in about 27.3 days, so its period is 27.3 days β‰ˆ one month. 1 1 37. 200 revolutions per minute is 200 minutes per revolution, so the period is 200 minutes, or 0.3 seconds.

38. Using the fact that 1 revolution = 2πœ‹ radians and 1 minute = 60 seconds, we have 200

rev rad 1 rad = (200) β‹… 2πœ‹ = 200 β‹… 2πœ‹ min min 60 sec (200)(6.283) β‰ˆ 60 β‰ˆ 20.94 radians per second.

Similarly, 500 rpm is equivalent to 52.36 radians per second. 39. The ramp in Figure 1.50 rises 1 ft over a horizontal distance of π‘₯ ft. (a) For a 1 ft rise over 12 ft, the angle in radians is πœƒ = arctan(1βˆ•12) = 0.0831. To find the angle in degrees, multiply by 180βˆ•πœ‹. Hence 1 180 arctan = 4.76β—¦ . πœƒ= πœ‹ 12 (b) We have 180 1 πœƒ= arctan = 7.13β—¦ . πœ‹ 8 (c) We have 180 1 πœƒ= arctan = 2.86β—¦ . πœ‹ 20 1 ft

πœƒ π‘₯ ft

Figure 1.50

PROBLEMS 40. (a) The period is 2πœ‹. (b) After πœ‹, the values of cos 2πœƒ repeat, but the values of 2 sin πœƒ do not (in fact, they repeat but flipped over the x-axis). After another πœ‹, that is after a total of 2πœ‹, the values of cos 2πœƒ repeat again, and now the values of 2 sin πœƒ repeat also, so the function 2 sin πœƒ + 3 cos 2πœƒ repeats at that point. 41. All three functions have amplitude 2 and period 2πœ‹. Each is just a horizontal shift of the others. (a) We see that β„Ž(𝑑) looks like a cosine graph with amplitude 2 and period 2πœ‹, but shifted right by πœ‹βˆ•2. Thus, β„Ž(𝑑) = 2 cos (𝑑 βˆ’ πœ‹βˆ•2). (b) We see that 𝑓 (𝑑) has and amplitude of 2 and a period of 2πœ‹. Furthermore, since 𝑓 (0) = 2, we know that 𝑓 (𝑑) = 2 cos 𝑑. (c) We see that 𝑔(𝑑) looks like a cosine graph with amplitude 2 and period 2πœ‹, but shifted left by πœ‹βˆ•2. Thus, 𝑔(𝑑) = 2 cos (𝑑 + πœ‹βˆ•2). 42. (a) The parameter 𝐴 is the amplitude of the function. Since the functions oscillate between βˆ’20 and +20, we have 𝐴 = 20. (b) We have 𝐡 = 2πœ‹βˆ•π‘ƒ , where 𝑃 is the period of the function. From the graphs, we see that the function repeats every 100 units, so the period is 100. Thus 𝐡 = 2πœ‹βˆ•100 = 0.0628. (c) Since cos 𝑑 has a maximum at 𝑑 = 0, the function 𝐴 cos((2πœ‹βˆ•100)𝑑) also achieves its maximum at 𝑑 = 0. Thus β„Ž = 0 corresponds to graph (II). The three graphs (I), (III), (IV) are all obtained by shifting graph (II) horizontally to the right. The size of the shift, β„Ž, can be determined by checking how far the first maximum on the graph has been shifted from the vertical axis. Graph (I) is shifted slightly more than 50, so graph (I) corresponds to β„Ž = 60. Similarly, graph (III) corresponds to β„Ž = 20 and graph (IV) to β„Ž = 50.


1.5 SOLUTIONS

57

43. The graph is a stretched sine function, so it starts at the midline, 𝑦 = 0, when π‘₯ = 0. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ and a maximum of π‘˜. Since π‘˜ is positive, the function begins by increasing. The period is 2πœ‹. See Figure 1.51. 𝑦 2πœ‹

π‘˜ βˆ’2πœ‹

2πœ‹ π‘˜

βˆ’π‘˜

π‘₯

βˆ’2πœ‹

Figure 1.51 44. The graph is a stretched cosine function reflected about the π‘₯-axis, so it starts at its minimum when π‘₯ = 0. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ and a maximum of π‘˜. The period is 2πœ‹. See Figure 1.52. 𝑦 2πœ‹

π‘˜

βˆ’2πœ‹

2πœ‹ π‘˜

βˆ’π‘˜

π‘₯

βˆ’2πœ‹

Figure 1.52 45. The graph is a stretched cosine function shifted vertically, so it starts at its maximum when π‘₯ = 0. We begin by finding the midline, which is π‘˜, since the sine function is shifted up by π‘˜. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of π‘˜ βˆ’ π‘˜ = 0 and a maximum of π‘˜ + π‘˜ = 2π‘˜. The period is 2πœ‹. See Figure 1.53. 𝑦 2πœ‹

π‘˜ βˆ’2πœ‹

βˆ’π‘˜

π‘˜

βˆ’2πœ‹

Figure 1.53

2πœ‹

π‘₯


58

Chapter One /SOLUTIONS

46. The graph is a stretched sine function shifted vertically, so it starts at its midline when π‘₯ = 0. We begin by finding the midline, which is βˆ’π‘˜, since the sine function is shifted up by βˆ’π‘˜ (down by π‘˜). The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ βˆ’ π‘˜ = βˆ’2π‘˜ and a maximum of βˆ’π‘˜ + π‘˜ = 0. Since π‘˜ is positive, the function begins by increasing. The period is 2πœ‹. See Figure 1.54. 𝑦 2πœ‹

π‘˜

βˆ’2πœ‹

2πœ‹ π‘˜

βˆ’π‘˜

π‘₯

βˆ’2πœ‹

Figure 1.54 47. The graph is a stretched sine function shifted horizontally. Since we have sin(π‘₯ βˆ’ π‘˜), the function is shifted π‘˜ units to the right, so the function takes on the value of its midline, 0, when π‘₯ = π‘˜. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ and a maximum of π‘˜. Since π‘˜ is positive, the function is increasing at π‘₯ = π‘˜. The period is 2πœ‹. See Figure 1.55. 𝑦 2πœ‹

π‘˜

βˆ’2πœ‹

2πœ‹

βˆ’π‘˜

π‘˜

π‘₯

βˆ’2πœ‹

Figure 1.55 48. The graph is a stretched cosine function shifted horizontally. Since we have cos(π‘₯ + π‘˜), the function is shifted βˆ’π‘˜ units to the right, which is π‘˜ units to the left, so the function takes on its maximum value when π‘₯ = βˆ’π‘˜. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ and a maximum of π‘˜. The period is 2πœ‹. See Figure 1.56. 𝑦 2πœ‹

π‘˜

βˆ’2πœ‹ βˆ’π‘˜

βˆ’2πœ‹

Figure 1.56

2πœ‹

π‘₯


1.5 SOLUTIONS

59

49. The graph is a vertically stretched sine function horizontally compressed by a factor of 2πœ‹βˆ•π‘˜. The function takes on the value of its midline, 0, when π‘₯ = 0. The amplitude is π‘˜, so the sinusoidal graph oscillates between a minimum of βˆ’π‘˜ and a maximum of π‘˜. Since π‘˜ is positive, the function is increasing at π‘₯ = 0. The period is 2πœ‹βˆ•(2πœ‹βˆ•π‘˜) = π‘˜. See Figure 1.57. 𝑦 2πœ‹

π‘˜ βˆ’π‘˜

βˆ’2πœ‹

π‘˜

2πœ‹

π‘₯

βˆ’2πœ‹

Figure 1.57 50. (a) Since 𝐢 represents the vertical shift, 𝐢 = 27.5β—¦ C, the average temperature. (b) The amplitude, 𝐴, is the distance above and below the midline at 𝐢, which represents the temperature variation above and below the average. Since the data rises 36.7 βˆ’ 27.5 = 9.2β—¦ C above 27.5β—¦ C, and falls 27.5 βˆ’ 18.4 = 9.1β—¦ C. We take 𝐴 to be the average 9.2 + 9.1 = 9.15β—¦ C. 𝐴= 2 (c) Since the period is 12 months, 2πœ‹ 12 = 𝐡 so 𝐡 = πœ‹βˆ•6. (d) The function is ( ) πœ‹ 𝑛 + 27.5. 𝐻(𝑛) = 9.15 cos 6 See Figure 1.58. temperature (β—¦ C) 36.7 27.5 18.4

1

3

5

7

9

11

𝑛 (months)

Figure 1.58 51. The parameter 𝐢 gives the midline of the graph. The minimum is at about 6 and the maximum is about 30; the midline is the average value. Thus 6 + 30 = 18β—¦ C. 𝐢= 2 52. The parameter 𝐴 gives the amplitude of the oscillation. The midline is at about 18 and the maximum is about 30, so the amplitude is the difference 𝐴 = 30 βˆ’ 18 = 12β—¦ C. 53. We have 𝐡 = 2πœ‹βˆ•π‘ƒ where 𝑃 is the period of the function. Since the period is 12 months, we have 𝐡 = 2πœ‹βˆ•12 = πœ‹βˆ•6.


60

Chapter One /SOLUTIONS

54. Since the maximum value of the function appears at about 𝑑 = 7.5, we see that the graph is obtained by horizontally shifting the graph of 𝐴 cos(𝐡𝑑) + 𝐢 to the right by 7.5 units. Thus β„Ž = 7.5 months. 55. The parameter 𝐢 gives the midline of the graph. The minimum is at about 175 and the maximum is about 725; the midline is the average value. Thus 175 + 725 = 450 thousand ft3 βˆ•sec. 𝐢= 2 56. The parameter 𝐴 gives the amplitude of the oscillation. The midline is about 450 and the maximum is about 725; the amplitude is the difference. Thus 𝐴 = 725 βˆ’ 450 = 275 thousand ft3 βˆ•sec. 57. We have 𝐡 = 2πœ‹βˆ•π‘ƒ where 𝑃 is the period of the function. Since the period is 12 months, we have 𝐡 = 2πœ‹βˆ•12 = πœ‹βˆ•6. 58. Since the graph increases across the midline at about 𝑑 = 1, we see that it is obtained by horizontally shifting the graph 𝐴 sin(𝐡𝑑) + 𝐢 to the right by 1 unit. Thus β„Ž = 1 month. 59. Over the one-year period, the average value is about 75β—¦ and the amplitude of the variation is about 90βˆ’60 = 15β—¦ . The 2 function assumes its minimum value right at the beginning of the year, so we want a negative cosine function. Thus, for 𝑑 in years, we have the function ) ( 2πœ‹ 𝑑 . 𝑓 (𝑑) = 75 βˆ’ 15 cos 12 (Many other answers are possible, depending on how you read the chart.) 60. sin π‘₯2 is by convention sin(π‘₯2 ), which means you square the π‘₯ first and then take the sine. sin2 π‘₯ = (sin π‘₯)2 means find sin π‘₯ and then square it. sin(sin π‘₯) means find sin π‘₯ and then take the sine of that. Expressing each as a composition: If 𝑓 (π‘₯) = sin π‘₯ and 𝑔(π‘₯) = π‘₯2 , then 2 sin π‘₯ = 𝑓 (𝑔(π‘₯)) sin2 π‘₯ = 𝑔(𝑓 (π‘₯)) sin(sin π‘₯) = 𝑓 (𝑓 (π‘₯)). 61. Suppose 𝑃 is at the point (3πœ‹βˆ•2, βˆ’1) and 𝑄 is at the point (5πœ‹βˆ•2, 1). Then Slope =

1 βˆ’ (βˆ’1) 2 = . 5πœ‹βˆ•2 βˆ’ 3πœ‹βˆ•2 πœ‹

If 𝑃 had been picked to the right of 𝑄, the slope would have been βˆ’2βˆ•πœ‹. 62. (a) See Figure 1.59.

900

𝑃

800 700 100 Jan. 1

Jul. 1

Jan. 1

𝑑 (months)

Figure 1.59 = 800, amplitude = 900βˆ’700 = 100, and period = 12 months, so 𝐡 = 2πœ‹βˆ•12 = (b) Average value of population = 700+900 2 2 πœ‹βˆ•6. Since the population is at its minimum when 𝑑 = 0, we use a negative cosine: ( ) πœ‹π‘‘ . 𝑃 = 800 βˆ’ 100 cos 6


1.5 SOLUTIONS 63. We use a cosine of the form

61

𝐻 = 𝐴 cos(𝐡𝑑) + 𝐢

and choose 𝐡 so that the period is 24 hours, so 2πœ‹βˆ•π΅ = 24 giving 𝐡 = πœ‹βˆ•12. The temperature oscillates around an average value of 60β—¦ F, so 𝐢 = 60. The amplitude of the oscillation is 20β—¦ F. To arrange that the temperature be at its lowest when 𝑑 = 0, we take 𝐴 negative, so 𝐴 = βˆ’20. Thus ( ) πœ‹ 𝐴 = 60 βˆ’ 20 cos 𝑑 . 12 64. The depth function is a vertical shift of a function of the form 𝐴 sin(𝐡𝑑). The vertical shift is 𝐴 = (5.5 + 8.5)βˆ•2 = 7. The amplitude is 𝐴 = 8.5 βˆ’ 7 = 1.5. The period is 6 = 2πœ‹βˆ•π΅ so 𝐡 = 2πœ‹βˆ•6 = πœ‹βˆ•3. Thus, we have ( ) πœ‹ 𝑑 . Depth = 7 + 1.5 sin 3 65. (a) Beginning at time 𝑑 = 0, the voltage will have oscillated through a complete cycle when cos(120πœ‹π‘‘) = cos(2πœ‹), hence when 𝑑 = 601 second. The period is 601 second. (b) 𝑉0 represents the amplitude of the oscillation. (c) See Figure 1.60. 𝑉 𝑉0

1 120

1 60

𝑑

Figure 1.60

66. (a) When the time is 𝑑 hours after 6 am, the solar panel outputs 𝑓 (𝑑) = 𝑃 (πœƒ(𝑑)) watts. So, ( ) πœ‹ 𝑓 (𝑑) = 10 sin 𝑑 14 where 0 ≀ 𝑑 ≀ 14 is the number of hours after 6 am. (b) The graph of 𝑓 (𝑑) is in Figure 1.61: 𝑃 (watts) 10

7

14

𝑑 (hrs after 6 am)

Figure 1.61 (c) The power output is greatest when sin(πœ‹π‘‘βˆ•14) = 1. Since 0 ≀ πœ‹π‘‘βˆ•14 ≀ πœ‹, the only point in the domain of 𝑓 at which sin(πœ‹π‘‘βˆ•14) = 1 is when πœ‹π‘‘βˆ•14 = πœ‹βˆ•2. Therefore, the power output is greatest when 𝑑 = 7, that is, at 1 pm. The output at this time will be 𝑓 (7) = 10 watts.


62

Chapter One /SOLUTIONS (d) On a typical winter day, there are 9 hours of sun instead of the 14 hours of sun. So, if 𝑑 is the number of hours since 8 am, the angle between a solar panel and the sun is πœ™=

πœ‹ 14 πœƒ= 𝑑 9 9

where 0 ≀ 𝑑 ≀ 9.

The solar panel outputs 𝑔(𝑑) = 𝑃 (πœ™(𝑑)) watts: 𝑔(𝑑) = 10 sin

(

πœ‹ 𝑑 9

)

where 0 ≀ 𝑑 ≀ 9 is the number of hours after 8 am. 67. The function 𝑅 has period of πœ‹, so its graph is as shown in Figure 1.62. The maximum value of the range is 𝑣20 βˆ•π‘” and occurs when πœƒ = πœ‹βˆ•4.

𝑣20

𝑅 𝑣2

𝑔

𝑅 = 𝑔0 sin 2πœƒ

πœ‹ 4

πœ‹ 2

πœƒ

Figure 1.62

68. (a) 𝑓 (𝑑) = βˆ’0.5 + sin 𝑑, 𝑔(𝑑) = 1.5 + sin 𝑑, β„Ž(𝑑) = βˆ’1.5 + sin 𝑑, π‘˜(𝑑) = 0.5 + sin 𝑑. (b) The values of 𝑔(𝑑) are one more than the values of π‘˜(𝑑), so 𝑔(𝑑) = 1 + π‘˜(𝑑). This happens because 𝑔(𝑑) = 1.5 + sin 𝑑 = 1 + 0.5 + sin 𝑑 = 1 + π‘˜(𝑑). (c) Since βˆ’1 ≀ sin 𝑑 ≀ 1, adding 1.5 everywhere we get 0.5 ≀ 1.5 + sin 𝑑 ≀ 2.5 and since 1.5 + sin 𝑑 = 𝑔(𝑑), we get 0.5 ≀ 𝑔(𝑑) ≀ 2.5. Similarly, βˆ’2.5 ≀ βˆ’1.5 + sin 𝑑 = β„Ž(𝑑) ≀ βˆ’0.5. 69. (a) The period of the tides is 2πœ‹βˆ•0.5 = 4πœ‹ = 12.566 hours. (b) The boat is afloat provided the water is deeper than 2.5 meters, so we need 𝑑(𝑑) = 5 + 4.6 sin(0.5𝑑) > 2.5. Figure 1.63 is a graph of 𝑑(𝑑), with time 𝑑 in hours since midnight, 0 ≀ 𝑑 ≀ 24. The boat leaves at 𝑑 = 12 (midday). To find the latest time the boat can return, we need to solve the equation 𝑑(𝑑) = 5 + 4.6 sin(0.5𝑑) = 2.5. A quick way to estimate the solution is to trace along the line 𝑦 = 2.5 in Figure 1.63 until we get to the first point of intersection to the right of 𝑑 = 12. The value we want is about 𝑑 = 20. Thus the water remains deep enough until about 8 pm. To find 𝑑 analytically, we solve 5 + 4.6 sin(0.5𝑑) = 2.5 2.5 = βˆ’0.5435 sin(0.5𝑑) = βˆ’ 4.6 1 arcsin(βˆ’0.5435) = βˆ’1.149. 𝑑= 0.5 This is the value of 𝑑 immediately to the left of the vertical axis. The water is also 2.5 meters deep one period later at 𝑑 = βˆ’1.149 + 12.566 = 11.417. This is shortly before the boat leaves, while the water is rising. We want the next time the time the water is this depth. The water was at its deepest (that is, 𝑑(𝑑) was a maximum) when 𝑑 = 12.566βˆ•4 = 3.142. From the figure, the time between when the water was 2.5 meters and when it was deepest was 3.142 + 1.149 = 4.291 hours. Thus, the value of 𝑑 that we want is 𝑑 = 11.417 + 2 β‹… 4.291 = 19.999.


1.5 SOLUTIONS depth in meters

63

𝑑(𝑑)

10 7.5 5 2.5 5

10

15

20

25

𝑑, hours since midnight

Figure 1.63 70. (a) 𝐷 = the average depth of the water. (b) 𝐴 = the amplitude = 15βˆ•2 = 7.5. (c) Period = 12.4 hours. Thus (𝐡)(12.4) = 2πœ‹ so 𝐡 = 2πœ‹βˆ•12.4 β‰ˆ 0.507. (d) 𝐢 is the time of a high tide. 71. Since 𝑏 is a positive constant, 𝑓 is a vertical shift of sin 𝑑 where the midline lies above the 𝑑-axis. So 𝑓 matches Graph 𝐢. Function 𝑔 is the sum of sin 𝑑 plus a linear function π‘Žπ‘‘ + 𝑏. We suspect then that the graph of 𝑔 might periodically oscillate about a line π‘Žπ‘‘ + 𝑏, just like the graph of sin 𝑑 oscillates about its midline. When adding π‘Žπ‘‘ + 𝑏 to sin 𝑑, we note that every zero of sin 𝑑, (𝑑, 0), gets displaced to a corresponding point (𝑑, π‘Žπ‘‘ + 𝑏) that lies both on the graph of 𝑔, and on the line π‘Žπ‘‘ + 𝑏. See Figure 1.64. So 𝑔 matches Graph 𝐡. Function β„Ž is the sum of sin 𝑑 plus an increasing exponential function 𝑒𝑐𝑑 + 𝑑. We suspect then that the graph of 𝑔 might periodically oscillate about the graph of 𝑒𝑐𝑑 + 𝑑, just like the graph of sin 𝑑 oscillates about its midline. When adding 𝑒𝑐𝑑 + 𝑑 to sin 𝑑, we note that every zero of sin 𝑑, (𝑑, 0), gets displaced to a corresponding point (𝑑, 𝑒𝑐𝑑 + 𝑑) that lies both on the graph of β„Ž, and on the graph of 𝑒𝑐𝑑 + 𝑑. See Figure 1.64. So β„Ž matches Graph 𝐴. Note that the oscillations on the graph of β„Ž may not be visible for all 𝑑 values. Function π‘Ÿ is the sum of sin 𝑑 plus a decreasing exponential function βˆ’π‘’π‘π‘‘ + 𝑏. We suspect then that the graph of π‘Ÿ might periodically oscillate about the graph of βˆ’π‘’π‘π‘‘ +𝑏, just like the graph of sin 𝑑 oscillates about its midline. When adding βˆ’π‘’π‘π‘‘ + 𝑏 to sin 𝑑, we note that every zero of sin 𝑑, (𝑑, 0), gets displaced to a corresponding point (𝑑, βˆ’π‘’π‘π‘‘ + 𝑏) that lies both on the graph of π‘Ÿ, and on the graph of βˆ’π‘’π‘π‘‘ + 𝑏. See Figure 1.64. So π‘Ÿ matches Graph 𝐷. Note that the oscillations on the graph of π‘Ÿ may not be visible for all 𝑑 values. 𝐴 𝐡 (𝑑, 𝑒𝑐𝑑 + 𝑏) (𝑑, π‘Žπ‘‘ + 𝑏) 𝐢 (𝑑, βˆ’π‘’π‘π‘‘ + 𝑏)

𝐷 (𝑑, 0)

𝑑

Figure 1.64 72. (a) The monthly mean CO2 increased about 12 ppm between December 2013 and December 2018. This is because the black curve shows that the December 2013 monthly mean was about 398 ppm, while the December 2018 monthly mean was about 410 ppm. The difference between these two values, 410 βˆ’ 398 = 12, gives the overall increase. (b) The average rate of increase is given by Average monthly increase of monthly mean =

1 410 βˆ’ 398 = ppm/month. 60 βˆ’ 0 5


64

Chapter One /SOLUTIONS This tells us that the slope of a linear equation approximating the black curve is 1βˆ•5. Since the vertical intercept is about 398, a possible equation for the approximately linear black curve is 𝑦=

1 𝑑 + 398, 5

where 𝑑 is measured in months since December 2013. (c) The period of the seasonal CO2 variation is about 12 months since this is approximately the time it takes for the function given by the blue curve to complete a full cycle. The amplitude is about 3.5 since, looking at the blue curve, the average distance between consecutive maximum and minimum values is about 7 ppm. So a possible sinusoidal function for the seasonal CO2 cycle is ( ) πœ‹ 𝑦 = 3.5 sin 𝑑 . 6 ( ) 1 πœ‹ 𝑑 and 𝑔(𝑑) = 𝑑 + 398, we have (d) Taking 𝑓 (𝑑) = 3.5 sin 6 5 ( ) 1 πœ‹ β„Ž(𝑑) = 3.5 sin 𝑑 + 𝑑 + 398. 6 5 See Figure 1.65. ppm 415 410 405 400 395

12

24

36

48

𝑑 (months since Dec 2013)

60

Figure 1.65

73. Figure 1.66 shows that the cross-sectional area is one rectangle of area β„Žπ‘€ and two triangles. Each triangle has height β„Ž and base π‘₯, where β„Ž β„Ž = tan πœƒ so π‘₯ = . π‘₯ tan πœƒ 1 β„Ž2 Area of triangle = π‘₯β„Ž = 2 2 tan πœƒ Total area = Area of rectangle + 2(Area of triangle) β„Ž2 β„Ž2 = β„Žπ‘€ + . = β„Žπ‘€ + 2 β‹… 2 tan πœƒ tan πœƒ

π‘₯πœƒ

πœƒ

6

π‘₯6πœƒ

β„Ž

β„Ž

?

𝑀

?πœƒ

Figure 1.66

74. (a) Two solutions: 0.4 and 2.7. See Figure 1.67. (b) arcsin(0.4) is the first solution approximated above; the second is an approximation to πœ‹ βˆ’ arcsin(0.4). (c) By symmetry, there are two solutions: βˆ’0.4 and βˆ’2.7.


1.5 SOLUTIONS

65

(d) βˆ’0.4 β‰ˆ βˆ’ arcsin(0.4) and βˆ’2.7 β‰ˆ βˆ’(πœ‹ βˆ’ arcsin(0.4)) = arcsin(0.4) βˆ’ πœ‹. 𝑦 1 0.4 βˆ’2.7

βˆ’0.4 0.4

π‘₯

2.7

βˆ’0.4 βˆ’1

Figure 1.67 75. (a) A table of values for 𝑔(π‘₯) is: π‘₯

βˆ’1

βˆ’0.8

βˆ’0.6

βˆ’0.4

βˆ’0.2

0

0.2

0.4

0.6

0.8

1

arccos π‘₯

3.14

2.50

2.21

1.98

1.77

1.57

1.37

1.16

0.93

0.64

0

(b) See Figure 1.68. πœ‹

𝑦 = arccos π‘₯

𝑦

6 Range

πœ‹ 2

βˆ’1

1

Domain

-

? π‘₯

Figure 1.68 1

βˆ’πœ‹βˆ•2

𝑦 𝑦 = cos π‘₯

πœ‹βˆ•2

πœ‹

π‘₯

βˆ’1

Figure 1.69 (c) The domain of arccos is βˆ’1 ≀ π‘₯ ≀ 1, because its inverse, cosine, takes all values from -1 to 1. The domains of arccos and arcsin are the same because their inverses, sine and cosine, have the same range. (d) Figure 1.68 shows that the range of 𝑦 = arccos π‘₯ is 0 ≀ πœƒ ≀ πœ‹. (e) The range of an inverse function is the domain of the original function. The arcsine is the inverse function to the piece of the sine having domain [βˆ’ πœ‹2 , πœ‹2 ]. Hence, the range of the arcsine is [βˆ’ πœ‹2 , πœ‹2 ]. But the piece of the cosine having domain [βˆ’ πœ‹2 , πœ‹2 ] does not have an inverse, because there are horizontal lines that intersect its graph twice. Instead, we define arccosine to be the inverse of the piece of cosine having domain [0, πœ‹], so the range of arccosine is [0, πœ‹], which is different from the range of arcsine. See Figure 1.69.

Strengthen Your Understanding 76. Scaling the output (that is, the function values, as in 𝑦 = 3 cos π‘₯) does not change the period but changes the amplitude. Scaling the input (that is, the independent variable, as in 𝑦 = cos 3π‘₯) changes the period of the function but not the amplitude. So 𝑓 has the same period, 2πœ‹, as cos π‘₯, but 𝑔 has a period smaller than 2πœ‹. See Figure 1.70.


66

Chapter One /SOLUTIONS 𝑓 (π‘₯) = 3 cos π‘₯

3 2 1 0 βˆ’1 βˆ’2 βˆ’3

𝑔(π‘₯) = cos 3π‘₯ 2πœ‹

4πœ‹

π‘₯

Figure 1.70

77. Increasing the value of 𝐡 decreases the period. For example, 𝑓 (π‘₯) = sin π‘₯ has period 2πœ‹, whereas 𝑔(π‘₯) = sin(2π‘₯) has period πœ‹. 78. The functions 𝑓 (π‘₯) = sin π‘₯ and 𝑔(π‘₯) = cos π‘₯ both have period 2πœ‹. The product, 𝑓 𝑔, of these two functions is periodic, but has a smaller period, πœ‹. See Figure 1.71. 𝑦 1

𝑦 = sin π‘₯ β‹… cos π‘₯

πœ‹

2πœ‹

π‘₯ 3πœ‹

βˆ’1

Figure 1.71

79. The maximum value of 𝐴 sin(𝐡π‘₯) is 𝐴, so the maximum value of 𝑦 = 𝐴 sin(𝐡π‘₯) + 𝐢 is 𝑦 = 𝐴 + 𝐢. 80. For 𝐡 > 0, the period of 𝑦 = sin(𝐡π‘₯) is 2πœ‹βˆ•π΅. Thus, we want 2πœ‹ = 23 𝐡

so

𝐡=

2πœ‹ . 23

The function is 𝑓 (π‘₯) = sin(2πœ‹π‘₯βˆ•23) 81. The midline is 𝑦 = (1200 + 2000)βˆ•2 = 1600 and the amplitude is 𝑦 = (2000 βˆ’ 1200)βˆ•2 = 400, so a possible function is 𝑓 (π‘₯) = 400(cos π‘₯) + 1600. 82. True. All functions in this family have period 2πœ‹ since the independent variable, π‘₯, (the input) is not scaled by a constant. The constant π‘Ž varies the amplitude of the functions in the family, but not the period. 83. False. Scaling the independent variable by a constant varies the period of the functions in the family. For a given value of π‘Ž, the period of the corresponding function in the family is 2πœ‹βˆ•π‘Ž. 84. False. The function cos πœƒ is decreasing and the function sin πœƒ is increasing. Thus, the function βˆ’ sin πœƒ is decreasing over this interval, which means 𝑓 is decreasing. 85. False. The period is 2πœ‹βˆ•(0.05πœ‹) = 40 86. True. The period is 2πœ‹βˆ•(200πœ‹) = 1βˆ•100 seconds. Thus, the function executes 100 cycles in 1 second. 87. False. If πœƒ = πœ‹βˆ•2, 3πœ‹βˆ•2, 5πœ‹βˆ•2 …, then πœƒ βˆ’ πœ‹βˆ•2 = 0, πœ‹, 2πœ‹ …, and the tangent is defined (it is zero) at these values. 88. False. When π‘₯ < 0, we have sin |π‘₯| = sin(βˆ’π‘₯) = βˆ’ sin π‘₯ β‰  sin π‘₯. 89. False. When πœ‹ < π‘₯ < 2πœ‹, we have sin |π‘₯| = sin π‘₯ < 0 but | sin π‘₯| > 0. 90. False. When πœ‹βˆ•2 < π‘₯ < 3πœ‹βˆ•2, we have cos |π‘₯| = cos π‘₯ < 0 but | cos π‘₯| > 0. 91. True. Since cos(βˆ’π‘₯) = cos π‘₯, cos |π‘₯| = cos π‘₯. 92. False. For example, sin(0) β‰  sin((2πœ‹)2 ), since sin(0) = 0 but sin((2πœ‹)2 ) = 0.98. 93. True. Since sin(πœƒ + 2πœ‹) = sin πœƒ for all πœƒ, we have 𝑔(πœƒ + 2πœ‹) = 𝑒sin(πœƒ+2πœ‹) = 𝑒sin πœƒ = 𝑔(πœƒ) for all πœƒ.


1.6 SOLUTIONS

67

94. False. A counterexample is given by 𝑓 (π‘₯) = sin π‘₯, which has period 2πœ‹, and 𝑔(π‘₯) = π‘₯2 . The graph of 𝑓 (𝑔(π‘₯)) = sin(π‘₯2 ) in Figure 1.72 is not periodic with period 2πœ‹.

1 βˆ’2πœ‹

βˆ’πœ‹

𝑦

βˆ’1

𝑓 (π‘₯) πœ‹

2πœ‹

π‘₯

Figure 1.72 95. True. If 𝑔(π‘₯) has period π‘˜, then 𝑔(π‘₯ + π‘˜) = 𝑔(π‘₯). Thus we have 𝑓 (𝑔(π‘₯ + π‘˜)) = 𝑓 (𝑔(π‘₯)) which shows that 𝑓 (𝑔(π‘₯)) is periodic with period π‘˜. 96. True, since | sin(βˆ’π‘₯)| = | βˆ’ sin π‘₯| = sin π‘₯. 97. False. If 𝑑 < βˆ’πœ‹βˆ•2 or 𝑑 > πœ‹βˆ•2, then sinβˆ’1 (sin 𝑑) β‰  𝑑. Note, however, that sinβˆ’1 (sin 𝑑) = 𝑑 for βˆ’πœ‹βˆ•2 ≀ 𝑑 ≀ πœ‹βˆ•2. 98. True. Since sin(𝑑 + 2πœ‹) = sin 𝑑, we have 𝑓 (𝑑 + 2πœ‹) = sinβˆ’1 (sin(𝑑 + 2πœ‹)) = sinβˆ’1 (sin 𝑑) = 𝑓 (𝑑). To see that this is the smallest interval on which we have a complete cycle, notice that since 𝑓 (𝑑) = 0 only for 𝑑 = π‘›πœ‹, 𝑛 = 0, Β±1, Β±2, …, the only possible period shorter than 2πœ‹ would be πœ‹. But 𝑓 (πœ‹βˆ•2)) = πœ‹βˆ•2 and 𝑓 (πœ‹βˆ•2 + πœ‹) = βˆ’πœ‹βˆ•2. Thus, πœ‹ is not a period.

Solutions for Section 1.6 EXERCISES 1. As π‘₯ β†’ ∞, 𝑦 β†’ ∞. As π‘₯ β†’ βˆ’βˆž, 𝑦 β†’ βˆ’βˆž. 2. As π‘₯ β†’ ∞, 𝑦 β†’ ∞. As π‘₯ β†’ βˆ’βˆž, 𝑦 β†’ 0. 3. Since 𝑓 (π‘₯) is an even power function with a negative leading coefficient, it follows that 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ +∞ and 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ βˆ’βˆž. 4. Since 𝑓 (π‘₯) is an odd power function with a positive leading coefficient, it follows that 𝑓 (π‘₯) β†’ +∞ as π‘₯ β†’ +∞ and 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ βˆ’βˆž. 5. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree term of 5π‘₯4 . Thus, as π‘₯ β†’ ±∞, we see that 𝑓 (π‘₯) β†’ +∞. 6. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree term of βˆ’5π‘₯3 . Thus, as π‘₯ β†’ +∞, we see that 𝑓 (π‘₯) β†’ βˆ’βˆž and as π‘₯ β†’ βˆ’βˆž, we see that 𝑓 (π‘₯) β†’ +∞. 7. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree 3π‘₯2 terms in the numerator and denominator. Thus, as π‘₯ β†’ ±∞, we see that 𝑓 (π‘₯) behaves like 2 = 3. We have 𝑓 (π‘₯) β†’ 3 π‘₯ as π‘₯ β†’ ±∞. 8. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree βˆ’3π‘₯3 = βˆ’3βˆ•2. We have terms in the numerator and denominator. Thus, as π‘₯ β†’ ±∞, we see that 𝑓 (π‘₯) behaves like 2π‘₯3 𝑓 (π‘₯) β†’ βˆ’3βˆ•2 as π‘₯ β†’ ±∞. 9. As π‘₯ β†’ ±∞, we see that 3π‘₯βˆ’4 gets closer and closer to 0, so 𝑓 (π‘₯) β†’ 0 as π‘₯ β†’ ±∞. 10. As π‘₯ β†’ +∞, we have 𝑓 (π‘₯) β†’ +∞. As π‘₯ β†’ βˆ’βˆž, we have 𝑓 (π‘₯) β†’ 0. 11. The power function with the higher power dominates as π‘₯ β†’ ∞, so 0.2π‘₯5 is larger.


68

Chapter One /SOLUTIONS

12. An exponential growth function always dominates a power function as π‘₯ β†’ ∞, so 10𝑒0.1π‘₯ is larger. 13. An exponential growth function always dominates a power function as π‘₯ β†’ ∞, so 1.05π‘₯ is larger. 14. The lower-power terms in a polynomial become insignificant as π‘₯ β†’ ∞, so we are comparing 2π‘₯4 to the leading term 10π‘₯3 . In comparing two power functions, the higher power dominates as π‘₯ β†’ ∞, so 2π‘₯4 is larger. 15. The lower-power terms in a polynomial become insignificant as π‘₯ β†’ ∞, so we are comparing the leading term 20π‘₯4 to the leading term 3π‘₯5 . In comparing two power functions, the higher power dominates as π‘₯ β†’ ∞, so the polynomial with leading term 3π‘₯5 is larger. As π‘₯ β†’ ∞, we see that 25 βˆ’ 40π‘₯2 + π‘₯3 + 3π‘₯5 is larger. √ 16. A power function with positive exponent dominates a log function, so as π‘₯ β†’ ∞, we see that π‘₯ is larger. 17. (I) (a) Minimum degree is 3 because graph turns around twice. (b) Leading coefficient is negative because 𝑦 β†’ βˆ’βˆž as π‘₯ β†’ ∞. (II) (a) Minimum degree is 4 because graph turns around three times. (b) Leading coefficient is positive because 𝑦 β†’ ∞ as π‘₯ β†’ ∞. (III) (a) Minimum degree is 4 because graph turns around three times. (b) Leading coefficient is negative because 𝑦 β†’ βˆ’βˆž as π‘₯ β†’ ∞. (IV) (a) Minimum degree is 5 because graph turns around four times. (b) Leading coefficient is negative because 𝑦 β†’ βˆ’βˆž as π‘₯ β†’ ∞. (V) (a) Minimum degree is 5 because graph turns around four times. (b) Leading coefficient is positive because 𝑦 β†’ ∞ as π‘₯ β†’ ∞. 18. (a) From the π‘₯-intercepts, we know the equation has the form 𝑦 = π‘˜(π‘₯ + 2)(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 5). Since 𝑦 = 2 when π‘₯ = 0, 2 = π‘˜(2)(βˆ’1)(βˆ’5) = π‘˜ β‹… 10 1 π‘˜= . 5 Thus we have

1 (π‘₯ + 2)(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 5). 5 19. (a) Because our cubic has a root at 2 and a double root at βˆ’2, it has the form 𝑦=

𝑦 = π‘˜(π‘₯ + 2)(π‘₯ + 2)(π‘₯ βˆ’ 2). Since 𝑦 = 4 when π‘₯ = 0, 4 = π‘˜(2)(2)(βˆ’2) = βˆ’8π‘˜, 1 π‘˜=βˆ’ . 2 Thus our equation is

1 𝑦 = βˆ’ (π‘₯ + 2)2 (π‘₯ βˆ’ 2). 2

20. 𝑓 (π‘₯) = π‘˜(π‘₯ + 3)(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 4) = π‘˜(π‘₯3 βˆ’ 2π‘₯2 βˆ’ 11π‘₯ + 12), where π‘˜ < 0. (π‘˜ β‰ˆ βˆ’ 16 if the horizontal and vertical scales are equal; otherwise one can’t tell how large π‘˜ is.) 21. 𝑓 (π‘₯) = π‘˜π‘₯(π‘₯ + 3)(π‘₯ βˆ’ 4) = π‘˜(π‘₯3 βˆ’ π‘₯2 βˆ’ 12π‘₯), where π‘˜ < 0. (π‘˜ β‰ˆ βˆ’ 29 if the horizontal and vertical scales are equal; otherwise one can’t tell how large π‘˜ is.) 22. 𝑓 (π‘₯) = π‘˜(π‘₯ + 2)(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3)(π‘₯ βˆ’ 5) = π‘˜(π‘₯4 βˆ’ 7π‘₯3 + 5π‘₯2 + 31π‘₯ βˆ’ 30), where π‘˜ > 0. (π‘˜ β‰ˆ 151 if the horizontal and vertical scales are equal; otherwise one can’t tell how large π‘˜ is.) 23. 𝑓 (π‘₯) = π‘˜(π‘₯ + 2)(π‘₯ βˆ’ 2)2 (π‘₯ βˆ’ 5) = π‘˜(π‘₯4 βˆ’ 7π‘₯3 + 6π‘₯2 + 28π‘₯ βˆ’ 40), where π‘˜ < 0. (π‘˜ β‰ˆ βˆ’ 151 if the scales are equal; otherwise one can’t tell how large π‘˜ is.) 24. There are only two functions, β„Ž and 𝑝, which can be put in the form 𝑦 = 𝐢𝑏π‘₯ , where 𝐢 and 𝑏 are constants: 𝑝(π‘₯) =

π‘Ž3 𝑏π‘₯ = (π‘Ž3 βˆ•π‘)𝑏π‘₯ , 𝑐

where 𝐢 = π‘Ž3 βˆ•π‘ since π‘Ž, 𝑐 are constants.

1 β„Ž(π‘₯) = βˆ’ π‘₯βˆ’2 = βˆ’5βˆ’(π‘₯βˆ’2) = βˆ’5βˆ’π‘₯+2 = (βˆ’25)5βˆ’π‘₯ . 5 Thus, β„Ž and 𝑝 are the only exponential functions.


1.6 SOLUTIONS

69

25. There is only one function, π‘Ÿ, who can be put in the form 𝑦 = 𝐴π‘₯2 + 𝐡π‘₯ + 𝐢: √ √ √ π‘Ÿ(π‘₯) = βˆ’π‘₯ + 𝑏 βˆ’ 𝑐π‘₯4 = βˆ’ 𝑐 π‘₯2 βˆ’ π‘₯ + 𝑏, where 𝐴 = βˆ’ 𝑐, since 𝑐 is a constant. Thus, π‘Ÿ is the only quadratic function. 26. There is only one function, π‘ž, which is linear. Function π‘ž is a constant linear function whose vertical intercept is the constant π‘Žπ‘2 βˆ•π‘, since π‘Ž, 𝑏 and 𝑐 are constants. 27. Since π‘Ž and 𝑏 are constants, so is π‘Žβˆ•π‘, so 𝑓 (π‘₯), which can be rewritten as 𝑓 (π‘₯) =

π‘Ž π‘₯ + 𝑐, 𝑏

is a polynomial function. Also, 𝑓 (π‘₯) is a rational function since it can be written as a quotient of polynomials with numerator 𝑓 (π‘₯) and denominator 1. On the other hand, 𝑓 (π‘₯) is not a power function since it is the sum of two terms with different powers of π‘₯, and as there are no terms with π‘₯ as an exponent, it cannot be an exponential function. Thus, 𝑓 (π‘₯) falls into families (III), and (IV). 28. By combining the two terms of 𝑔(π‘₯) over a common denominator, 𝑔(π‘₯) can be rewritten as 𝑔(π‘₯) = π‘Žπ‘₯2 +

𝑏 π‘Žπ‘₯4 𝑏 π‘Žπ‘₯4 + 𝑏 = 2 + 2 = . 2 π‘₯ π‘₯ π‘₯ π‘₯2

Therefore, since 𝑔(π‘₯) can be written as a quotient of polynomials, it is a rational function. However, 𝑔(π‘₯) is not a power function since it is the sum of two terms with different powers of π‘₯, it is not a polynomial since it has terms with negative powers of π‘₯, and as there are no terms with π‘₯ as an exponent, it cannot be an exponential function. Thus, 𝑔(π‘₯) falls into family (IV) only. 29. Since 𝑏 and 𝑐 are constants, so is π‘βˆ•π‘ π‘Ž . In addition, since π‘Ž is a positive integer, β„Ž(π‘₯), which can be rewritten as ( )π‘Ž 𝑏 π‘₯ β„Ž(π‘₯) = 𝑏 = π‘Ž π‘₯π‘Ž , 𝑐 𝑐 is a power function. It is also a polynomial, since a polynomial is a sum of power functions with positive integer exponents, and it is a rational function, since any polynomial can be viewed as a rational function with denominator 1. However, β„Ž(π‘₯) is not an exponential function. Thus, β„Ž(π‘₯) falls into families (II), (III) and (IV). 30. Since π‘Ž is constant, π‘˜(π‘₯) is a power function. Since π‘Ž is a positive integer and a polynomial is a sum of power functions with non-negative integer powers, π‘˜(π‘₯) is a polynomial. Also, π‘˜(π‘₯) is a rational function as it is the quotient of the two polynomials 𝑏π‘₯π‘Ž and 1. On the other hand, π‘˜(π‘₯) is not exponential since there are no terms with π‘₯ as an exponent. Thus, π‘˜(π‘₯) falls into families (II), (III), and (IV). 31. Since π‘Ž and 𝑏 are constants, so is π‘Ž + 𝑏, so 𝑗(π‘₯), which can be written in the form 𝑗(π‘₯) = π‘Žπ‘₯βˆ’1 +

𝑏 = π‘Žπ‘₯βˆ’1 + 𝑏π‘₯βˆ’1 = (π‘Ž + 𝑏)π‘₯βˆ’1 , π‘₯

is a power function. We can also write 𝑗(π‘₯) as 𝑗(π‘₯) = (π‘Ž + 𝑏)π‘₯βˆ’1 =

π‘Ž+𝑏 , π‘₯

a quotient of polynomials, so it is also a rational function. The function 𝑗(π‘₯) is not a polynomial as there are terms with negative powers of π‘₯, and 𝑗(π‘₯) is not exponential since there are no terms with π‘₯ as an exponent. Thus, 𝑗(π‘₯) falls into families (II), and (IV). 32. Since π‘Ž, 𝑏, and 𝑐 are all constants, so is ((π‘Ž + 𝑏)βˆ•π‘)2 , so 𝑙(π‘₯), which can be written in the form (( ) ) )π‘₯ ( π‘Ž+𝑏 2 π‘Ž + 𝑏 2π‘₯ = , 𝑙(π‘₯) = 𝑐 𝑐 is an exponential function. It is neither a polynomial, rational, nor power function since there is a variable in the exponent of one of the terms. Thus, 𝑙(π‘₯) falls into family (I). 33. Only IV is of degree 3, because the highest degree term is π‘₯3 . Expanding shows the other polynomials have different degrees.


70

Chapter One /SOLUTIONS

34. III and VI, since expanding gives

𝑦 = π‘₯4 βˆ’ 2π‘₯2 + 1

and

𝑦 = π‘₯4 βˆ’ 4.

35. I, II, and V. Both I and II are the ratios of polynomials; V can be rewritten as the ratio of polynomials as: 𝑦=

π‘₯2 βˆ’ 1 . π‘₯

Since in each case, the denominator is not a constant, these functions cannot be thought of as polynomials. √ 36. I, since the numerator has two zeros, π‘₯ = Β± 2. III, since the polynomial factors to 𝑦 = βˆ’(π‘₯ βˆ’ 1)2 (π‘₯ + 1)2 , it has two zeros, π‘₯ = Β±1. π‘₯2 βˆ’ 1 V, since we can combine terms, 𝑦 = , and the numerator has two zeros, π‘₯ = Β±1. π‘₯ √ 2 2 VI, since 𝑦 = (π‘₯ βˆ’ 2)(π‘₯ + 2) has two distinct zeros, π‘₯ = Β± 2, from the first factor. The second factor does not contribute any zeros. 37. V, since the denominator has exactly one zero, π‘₯ = 0. 38. IV, since it factors to 𝑦 = π‘₯(π‘₯ βˆ’ 1)(π‘₯ + 1).

√ 39. II, since the denominator has two zeros, π‘₯ = Β± 2. 40. I and II, since in each case as π‘₯ β†’ ∞ or π‘₯ β†’ βˆ’βˆž, we have 𝑦→𝑦=

π‘₯2 = 1. π‘₯2

41. We have Zeros: π‘₯ = 1, π‘₯ = 2, π‘₯ = 3 Asymptotes: None.

42. We have Zeros: π‘₯ = 3 Asymptotes: π‘₯ = 1, π‘₯ = 2. 43. We have Zeros: π‘₯ = 1, π‘₯ = 3 Asymptotes: π‘₯ = 2. 44. We combine the fractions 2(π‘₯ βˆ’ 2) 1 π‘₯βˆ’3+π‘₯βˆ’1 2π‘₯ βˆ’ 4 1 + = = = π‘₯βˆ’1 π‘₯βˆ’3 (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3) (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3) (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3) Thus, Zeros: π‘₯ = 2 Asymptotes: π‘₯ = 1, π‘₯ = 3. 45. Since the graph of this function is only defined for positive values of π‘₯, this is the graph of a logarithmic function. 46. Since the graph of this function has only one horizontal asymptote, this is the graph of an exponential function. 47. Since the graph of this function has two horizontal asymptotes, it must be a rational function. 48. Since this function both increases and decreases over different parts of its domain, it must be a rational function.


1.6 SOLUTIONS

71

PROBLEMS 49. Consider the end behavior of the graph; that is, as π‘₯ β†’ +∞ and π‘₯ β†’ βˆ’βˆž. The ends of a degree 5 polynomial are in Quadrants I and III if the leading coefficient is positive or in Quadrants II and IV if the leading coefficient is negative. Thus, there must be at least one root. Since the degree is 5, there can be no more than 5 roots. Thus, there may be 1, 2, 3, 4, or 5 roots. Graphs showing these five possibilities are shown in Figure 1.73. (a) 5 roots

(b) 4 roots

(c) 3 roots

π‘₯

(d) 2 roots

π‘₯

(e) 1 root π‘₯

π‘₯

π‘₯

Figure 1.73 50. The graphs of both these functions will resemble that of π‘₯3 on a large enough window. One way to tackle the problem is to graph them both (along with π‘₯3 if you like) in successively larger windows until the graphs come together. In Figure 1.74, 𝑓 , 𝑔 and π‘₯3 are graphed in four windows. In the largest of the four windows the graphs are indistinguishable, as required. Answers may vary. 𝑦

𝑦

106

109

βˆ’100

100

π‘₯

βˆ’1000

βˆ’106

1000

βˆ’109 𝑦

𝑦

1012

βˆ’104

π‘₯

1015

104

π‘₯

βˆ’105

βˆ’1012

105

π‘₯

βˆ’1015

Figure 1.74 51. The function is a cubic polynomial with positive leading coefficient. Since the figure given in the text shows that the function turns around once, we know that the function has the shape shown in Figure 1.75. The function is below the π‘₯-axis for π‘₯ = 5 in the given graph, and we know that it goes to +∞ as π‘₯ β†’ +∞ because the leading coefficient is positive. Therefore, there are exactly three zeros. Two zeros are shown, and occur at approximately π‘₯ = βˆ’1 and π‘₯ = 3. The third zero must be to the right of π‘₯ = 10 and so occurs for some π‘₯ > 10.

Figure 1.75


72

Chapter One /SOLUTIONS

52. (a)

(i) If (1, 1) is on the graph, we know that 1 = π‘Ž(1)2 + 𝑏(1) + 𝑐 = π‘Ž + 𝑏 + 𝑐. (ii) If (1, 1) is the vertex, then the axis of symmetry is π‘₯ = 1, so βˆ’

𝑏 = 1, 2π‘Ž

and thus

𝑏 π‘Ž = βˆ’ , so 𝑏 = βˆ’2π‘Ž. 2 But to be the vertex, (1, 1) must also be on the graph, so we know that π‘Ž + 𝑏 + 𝑐 = 1. Substituting 𝑏 = βˆ’2π‘Ž, we get βˆ’π‘Ž + 𝑐 = 1, which we can rewrite as π‘Ž = 𝑐 βˆ’ 1, or 𝑐 = 1 + π‘Ž. (iii) For (0, 6) to be on the graph, we must have 𝑓 (0) = 6. But 𝑓 (0) = π‘Ž(02 ) + 𝑏(0) + 𝑐 = 𝑐, so 𝑐 = 6. (b) To satisfy all the conditions, we must first, from (a)(iii), have 𝑐 = 6. From (a)(ii), π‘Ž = 𝑐 βˆ’ 1 so π‘Ž = 5. Also from (a)(ii), 𝑏 = βˆ’2π‘Ž, so 𝑏 = βˆ’10. Thus the completed equation is 𝑦 = 𝑓 (π‘₯) = 5π‘₯2 βˆ’ 10π‘₯ + 6, which satisfies all the given conditions. 53. Let us represent the height by β„Ž. Since the volume is 𝑉 , we have π‘₯2 β„Ž = 𝑉 . Solving for β„Ž gives

𝑉 . π‘₯2 The graph is in Figure 1.76. We are assuming 𝑉 is a positive constant. β„Ž=

β„Ž

β„Ž = 𝑉 βˆ•π‘₯2 π‘₯

Figure 1.76

54. (a) Let the height of the can be β„Ž. Then

𝑉 = πœ‹π‘Ÿ2 β„Ž.

The surface area consists of the area of the ends (each is πœ‹π‘Ÿ2 ) and the curved sides (area 2πœ‹π‘Ÿβ„Ž), so 𝑆 = 2πœ‹π‘Ÿ2 + 2πœ‹π‘Ÿβ„Ž. Solving for β„Ž from the formula for 𝑉 , we have β„Ž= Substituting into the formula for 𝑆, we get 𝑆 = 2πœ‹π‘Ÿ2 + 2πœ‹π‘Ÿ β‹…

𝑉 . πœ‹π‘Ÿ2 𝑉 2𝑉 = 2πœ‹π‘Ÿ2 + . π‘Ÿ πœ‹π‘Ÿ2

(b) For large π‘Ÿ, the 2𝑉 βˆ•π‘Ÿ term becomes negligible, meaning 𝑆 β‰ˆ 2πœ‹π‘Ÿ2 , and thus 𝑆 β†’ ∞ as π‘Ÿ β†’ ∞.


1.6 SOLUTIONS

73

(c) The graph is in Figure 1.77. 𝑆 100 75 𝑆 = 2πœ‹π‘Ÿ2 + 2π‘‰π‘Ÿ 𝑉 = 10

50 25 0

1

2

3

4

5

π‘Ÿ

Figure 1.77 55. Substituting 𝑀 = 65 and β„Ž = 160, we have (a)

𝑠 = 0.01(650.25 )(1600.75 ) = 1.3 m2 .

(b) We substitute 𝑠 = 1.5 and β„Ž = 180 and solve for 𝑀: 1.5 = 0.01𝑀0.25 (1800.75 ). We have

1.5 = 3.05. 0.01(1800.75 ) Since 𝑀0.25 = 𝑀1βˆ•4 , we take the fourth power of both sides, giving 𝑀0.25 =

𝑀 = 86.8 kg. (c) We substitute 𝑀 = 70 and solve for β„Ž in terms of 𝑠: 𝑠 = 0.01(700.25 )β„Ž0.75 , so

𝑠 . 0.01(700.25 ) Since β„Ž0.75 = β„Ž3βˆ•4 , we take the 4βˆ•3 power of each side, giving )4βˆ•3 ( 𝑠 𝑠4βˆ•3 β„Ž= = 0.01(700.25 ) (0.014βˆ•3 )(701βˆ•3 ) β„Ž0.75 =

so

β„Ž = 112.6𝑠4βˆ•3 .

56. Let 𝐷(𝑣) be the stopping distance required by an Alpha Romeo as a function of its velocity. The assumption that stopping distance is proportional to the square of velocity is equivalent to the equation 𝐷(𝑣) = π‘˜π‘£2 where π‘˜ is a constant of proportionality. To determine the value of π‘˜, we use the fact that 𝐷(70) = 148. 𝐷(70) = π‘˜(70)2 = 148. Thus,

148 β‰ˆ 0.0302. 702 ) ( 148 148 = 37 ft (35)2 = 𝐷(35) = 4 702 π‘˜=

It follows that

and

) 148 (140)2 = 148 β‹… 4 = 592 ft. 2 70 Thus, at half the speed it requires one fourth the distance, whereas at twice the speed it requires four times the distance, as we would expect from the equation. (We could in fact have figured it out that way, without solving for π‘˜ explicitly.) 𝐷(140) =

(


74

Chapter One /SOLUTIONS

57. (a) Since the rate 𝑅 varies directly with the fourth power of the radius π‘Ÿ, we have the formula 𝑅 = π‘˜π‘Ÿ4 where π‘˜ is a constant. (b) Given 𝑅 = 400 for π‘Ÿ = 3, we can determine the constant π‘˜. 400 = π‘˜(3)4 400 = π‘˜(81) 400 β‰ˆ 4.93827. π‘˜= 81 So the formula is

𝑅 = 4.93827π‘Ÿ4

(c) Evaluating the formula above at π‘Ÿ = 5 yields 𝑅 = 4.93827(5)4 = 3086.42

cm3 . sec

58. The pomegranate is at ground level when 𝑓 (𝑑) = βˆ’16𝑑2 + 64𝑑 = βˆ’16𝑑(𝑑 βˆ’ 4) = 0, so when 𝑑 = 0 or 𝑑 = 4. At time 𝑑 = 0 it is thrown, so it must hit the ground at 𝑑 = 4 seconds. The symmetry of its path with respect to time may convince you that it reaches its maximum height after 2 seconds. Alternatively, we can think of the graph of 𝑓 (𝑑) = βˆ’16𝑑2 + 64𝑑 = βˆ’16(𝑑 βˆ’ 2)2 + 64, which is a downward parabola with vertex (i.e., highest point) at (2, 64). The maximum height is 𝑓 (2) = 64 feet. 59. (a) The object starts at 𝑑 = 0, when 𝑠 = 𝑣0 (0) βˆ’ 𝑔(0)2 βˆ•2 = 0. Thus it starts on the ground, with zero height. (b) The object hits the ground when 𝑠 = 0. This is satisfied at 𝑑 = 0, before it has left the ground, and at some later time 𝑑 that we must solve for. ( ) 0 = 𝑣0 𝑑 βˆ’ 𝑔𝑑2 βˆ•2 = 𝑑 𝑣0 βˆ’ π‘”π‘‘βˆ•2 Thus 𝑠 = 0 when 𝑑 = 0 and when 𝑣0 βˆ’ π‘”π‘‘βˆ•2 = 0, i.e., when 𝑑 = 2𝑣0 βˆ•π‘”. The starting time is 𝑑 = 0, so it must hit the ground at time 𝑑 = 2𝑣0 βˆ•π‘”. (c) The object reaches its maximum height halfway between when it is released and when it hits the ground, or at 𝑑 = (2𝑣0 βˆ•π‘”)βˆ•2 = 𝑣0 βˆ•π‘”. (d) Since we know the time at which the object reaches its maximum height, to find the height it actually reaches we just use the given formula, which tells us 𝑠 at any given 𝑑. Substituting 𝑑 = 𝑣0 βˆ•π‘”, ( ) ( ) 𝑣20 𝑣20 𝑣20 𝑣0 1 = βˆ’ 𝑔 βˆ’ 𝑠 = 𝑣0 𝑔 2 𝑔 2𝑔 𝑔2 =

2𝑣20 βˆ’ 𝑣20 2𝑔

=

𝑣20 2𝑔

.

60. (a) 𝑅(𝑃 ) = π‘˜π‘ƒ (𝐿 βˆ’ 𝑃 ), where π‘˜ is a positive constant. (b) A possible graph is in Figure 1.78. 𝑅

𝐿

Figure 1.78

𝑃


1.6 SOLUTIONS

75

61. Yes. The graph of this power function is increasing and concave down for positive mass 𝑀. See Figure 1.79. This function could represent the length of a plant species that stretches relatively less per unit mass increase as the plant gets larger. 𝐿 𝐿 = 2𝑀 1βˆ•4

𝑀

Figure 1.79 62. No. The graph of this polynomial function is increasing but concave up for positive mass 𝑀. See Figure 1.80. A plant growing according to this function would stretch relatively more (not less) per unit mass increase as the plant gets larger. 𝐿

𝐿 = 0.2𝑀 3 + 𝑀 4 𝑀

Figure 1.80 63. No. The graph of this power function is decreasing for positive mass 𝑀. See Figure 1.81. A plant growing according to this function would actually shrink in length (rather than stretch) as its mass increases. Furthermore, when the mass approaches zero, the length approaches a positive number, not zero. 𝐿

𝐿 = 2𝑀 βˆ’1βˆ•4

𝑀

Figure 1.81 64. Yes. The graph of this rational function is increasing and concave down. See Figure 1.82. A plant species growing according to this function stretches relatively less per unit mass increase as the plant gets larger. 𝐿 𝐿=

4(𝑀 + 1)2 βˆ’ 4 (𝑀 + 1)2

𝑀

Figure 1.82


76

Chapter One /SOLUTIONS

65. No. The graph of this rational function is decreasing for positive mass 𝑀. See Figure 1.83. A plant growing according to this function would actually shrink in length (rather than stretch) as its mass increases. Furthermore, when the mass approaches zero, the length approaches a positive number, not zero. 𝐿

𝐿=

10(𝑀 + 1)2 βˆ’ 1 (𝑀 + 1)3 𝑀

Figure 1.83

66. To find the horizontal asymptote, we look at end behavior. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π‘₯ β†’ ±∞, we see that 5 5π‘₯ = . 𝑓 (π‘₯) β†’ 2π‘₯ 2 There is a horizontal asymptote at 𝑦 = 5βˆ•2. To find the vertical asymptotes, we set the denominator equal to zero. When 2π‘₯ + 3 = 0, we have π‘₯ = βˆ’3βˆ•2 so there is a vertical asymptote at π‘₯ = βˆ’3βˆ•2. 67. To find the horizontal asymptote, we look at end behavior. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π‘₯ β†’ ±∞, we see that π‘₯2 𝑓 (π‘₯) β†’ 2 = 1. π‘₯ There is a horizontal asymptote at 𝑦 = 1. To find the vertical asymptotes, we set the denominator equal to zero. When π‘₯2 βˆ’ 4 = 0, we have π‘₯ = Β±2 so there are vertical asymptotes at π‘₯ = βˆ’2 and at π‘₯ = 2. 68. To find the horizontal asymptote, we look at end behavior. As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π‘₯ β†’ ±∞, we see that 5π‘₯3 𝑓 (π‘₯) β†’ 3 = 5. π‘₯ There is a horizontal asymptote at 𝑦 = 5. To find the vertical asymptotes, we set the denominator equal to zero. When π‘₯3 βˆ’ 27 = 0, we have π‘₯ = 3 so there is a vertical asymptote at π‘₯ = 3. 69. (a) A polynomial has the same end behavior as its leading term, so this polynomial behaves as βˆ’5π‘₯4 globally. Thus we have: 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ βˆ’βˆž, and 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ +∞. (b) Polynomials behave globally as their leading term, so this rational function behaves globally as (3π‘₯2 )βˆ•(2π‘₯2 ), or 3βˆ•2. Thus we have: 𝑓 (π‘₯) β†’ 3βˆ•2 as π‘₯ β†’ βˆ’βˆž, and 𝑓 (π‘₯) β†’ 3βˆ•2 as π‘₯ β†’ +∞. (c) We see from a graph of 𝑦 = 𝑒π‘₯ that 𝑓 (π‘₯) β†’ 0 as π‘₯ β†’ βˆ’βˆž, and 𝑓 (π‘₯) β†’ +∞ as π‘₯ β†’ +∞. 70. 𝑔(π‘₯) = 2π‘₯2 , β„Ž(π‘₯) = π‘₯2 + π‘˜ for any π‘˜ > 0. Notice that the graph is symmetric about the 𝑦-axis and limπ‘₯β†’βˆž 𝑓 (π‘₯) = 2. 71. We use the fact that at a constant speed, Time = Distanceβˆ•Speed. Thus, Total time = Time running + Time walking 3 6 = + . π‘₯ π‘₯βˆ’2 Horizontal asymptote: π‘₯-axis. Vertical asymptote: π‘₯ = 0 and π‘₯ = 2.


1.6 SOLUTIONS

77

72. (a) II and III because in both cases, the numerator and denominator each have π‘₯2 as the highest power, with coefficient = 1. Therefore, π‘₯2 𝑦 β†’ 2 = 1 as π‘₯ β†’ ±∞. π‘₯ (b) I, since π‘₯ 𝑦 β†’ 2 = 0 as π‘₯ β†’ ±∞. π‘₯ (c) II and III, since replacing π‘₯ by βˆ’π‘₯ leaves the graph of the function unchanged. (d) None (e) III, since the denominator is zero and 𝑓 (π‘₯) tends to ±∞ when π‘₯ = Β±1. 73. β„Ž(𝑑) cannot be of the form 𝑐𝑑2 or π‘˜π‘‘3 since β„Ž(0.0) = 2.04. Therefore β„Ž(𝑑) must be the exponential, and we see that the ratio of successive values of β„Ž is approximately 1.5. Therefore β„Ž(𝑑) = 2.04(1.5)𝑑 . If 𝑔(𝑑) = 𝑐𝑑2 , then 𝑐 = 3 since 𝑔(1.0) = 3.00. However, 𝑔(2.0) = 24.00 β‰  3 β‹… 22 . Therefore 𝑔(𝑑) = π‘˜π‘‘3 , and using 𝑔(1.0) = 3.00, we obtain 𝑔(𝑑) = 3𝑑3 . Thus 𝑓 (𝑑) = 𝑐𝑑2 , and since 𝑓 (2.0) = 4.40, we have 𝑓 (𝑑) = 1.1𝑑2 . 74. The graphs are shown in Figure 1.84. 𝑦

(a) 9

𝑦

(b) π‘₯4

3π‘₯

50000

π‘₯4

3π‘₯

5

𝑦

(c)

625

π‘₯

5

3π‘₯

π‘₯4 π‘₯

10

π‘₯

Figure 1.84 75. Since the parabola opens upward, we must have π‘Ž > 0. To determine a relationship between π‘₯ and 𝑦 at the point of intersection 𝑃 , we eliminate π‘Ž from the parabola and circle equations. Since 𝑦 = π‘₯2 βˆ•π‘Ž, we have π‘Ž = π‘₯2 βˆ•π‘¦. Putting this into the circle equation gives π‘₯2 + 𝑦2 = 2π‘₯4 βˆ•π‘¦2 . Rewrite this as π‘₯2 𝑦2 + 𝑦4 = 2π‘₯4 𝑦4 + π‘₯2 𝑦2 βˆ’ 2π‘₯4 = 0 2

(𝑦 + 2π‘₯2 )(𝑦2 βˆ’ π‘₯2 ) = 0. This means π‘₯2 = 𝑦2 (since 𝑦2 cannot equal βˆ’2π‘₯2 ). Thus π‘₯ = 𝑦 since 𝑃 is in the first quadrant. So 𝑃 moves out along the line 𝑦 = π‘₯ through the origin. 76. (a) The graph is shown in Figure 1.85. The graph represented by the exact formula has a vertical asymptote where the denominator is undefined. This happens when 𝑣2 = 0, or at 𝑣2 = 𝑐 2 . 𝑐2 Since 𝑣 > 0, the graph of the exact formula has a vertical asymptote where 1βˆ’

𝑣 = 𝑐 = 3 β‹… 108 m/sec. 𝐸 (1017 joules)

(

5

𝐸 = π‘šπ‘ 2

4

1 √ βˆ’1 1βˆ’π‘£2 βˆ•π‘ 2

3 2

𝐸 = 12 π‘šπ‘£2

1 1

2

3

4

5

Figure 1.85

𝑣 (108 m/sec)

)


78

Chapter One /SOLUTIONS (b) The first formula does not give a good approximation to the exact formula when the graphs are not close together. This happens for 𝑣 > 1.5 β‹… 108 m/sec. For 𝑣 < 1.5 β‹… 108 m/sec, the graphs look close together. However, the vertical scale we are using is so large and the graphs are so close to the 𝑣-axis that a more careful analysis should be made. We should zoom in and redraw the graph.

77. Since 𝑧 = ln π‘₯, we have π‘₯ = 𝑒𝑧 . Hence 𝑦 = 100π‘₯βˆ’0.2 = 100(𝑒𝑧 )βˆ’0.2 = 100π‘’βˆ’0.2𝑧 .

Strengthen Your Understanding 78. The graph of a polynomial of degree 5 cuts the horizontal axis at most five times, but it could be fewer. For example, 𝑓 (π‘₯) = π‘₯5 cuts the π‘₯-axis only once. 79. A fourth degree polynomial tends to negative infinity if the leading coefficient (coefficient of the π‘₯4 term) is negative. For example, 𝑓 (π‘₯) = βˆ’π‘₯4 tends to negative infinity as π‘₯ β†’ ∞. 80. A rational function has no vertical asymptotes if the denominator has no zeros. For example: 𝑓 (π‘₯) =

1 . π‘₯2 + 1

81. As seen from the graphs of the functions in Figure 1.86, this inequality only holds for π‘₯ > 1. The functions cross at the point (1, 1) and the inequality is reversed for 0 < π‘₯ < 1. 𝑦 𝑦 = π‘₯5

3

𝑦 = π‘₯3

2 1 0.5

1

1.5

π‘₯

Figure 1.86

82. The rational function 𝑓 (π‘₯) = (π‘₯3 + 1)βˆ•π‘₯ has no horizontal asymptotes. To see this, observe that 𝑦 = 𝑓 (π‘₯) =

π‘₯3 π‘₯3 + 1 β‰ˆ = π‘₯2 π‘₯ π‘₯

for large π‘₯. Thus, 𝑦 β†’ ∞ as π‘₯ β†’ ±∞. 83. Let 𝑓 (π‘₯) = π‘₯βˆ•(π‘₯2 + 1). Since

π‘₯ 1 π‘₯ β‰ˆ 2 = for large π‘₯, π‘₯ π‘₯2 + 1 π‘₯ and 1βˆ•π‘₯ β†’ 0 as π‘₯ β†’ ∞, the function 𝑓 (π‘₯) has horizontal asymptote 𝑦 = 0. We have 𝑓 (0) = 0, so 𝑓 (π‘₯) crosses this asymptote at π‘₯ = 0. 𝑦=

84. One possibility is 𝑝(π‘₯) = (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 2)(π‘₯ βˆ’ 3) = π‘₯3 βˆ’ 6π‘₯2 + 11π‘₯ βˆ’ 6. 85. A possible function is 𝑓 (π‘₯) =

3π‘₯ . π‘₯ βˆ’ 10

𝑓 (π‘₯) =

1 . π‘₯2 + 1

86. One possibility is


1.6 SOLUTIONS

79

1 . Other answers are possible. π‘₯ + 7πœ‹ 1 . This function has an asymptote corresponding to every factor in 88. Let 𝑓 (π‘₯) = (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 2)(π‘₯ βˆ’ 3) β‹― (π‘₯ βˆ’ 16)(π‘₯ βˆ’ 17) the denominator. Other answers are possible. π‘₯βˆ’1 89. The function 𝑓 (π‘₯) = has 𝑦 = 1 as the horizontal asymptote and π‘₯ = 2 as the vertical asymptote. These lines cross π‘₯βˆ’2 at the point (2, 1). Other answers are possible.

87. Let 𝑓 (π‘₯) =

90. False. The polynomial 𝑓 (π‘₯) = π‘₯2 + 1, with degree 2, has no real zeros. 91. True. If the degree of the polynomial, 𝑝(π‘₯), is 𝑛, then the leading term is π‘Žπ‘› π‘₯𝑛 with π‘Žπ‘› β‰  0. If 𝑛 is odd and π‘Žπ‘› is positive, 𝑝(π‘₯) tends toward ∞ as π‘₯ β†’ ∞ and 𝑝(π‘₯) tends toward βˆ’βˆž as π‘₯ β†’ βˆ’βˆž. Since the graph of 𝑝(π‘₯) has no breaks in it, the graph must cross the π‘₯-axis at least once. If 𝑛 is odd and π‘Žπ‘› is negative, a similar argument applies, with the signs reversed, but leading to the same conclusion. 92. False. Suppose 𝑓 (π‘₯) = 𝑔(π‘₯) = π‘₯2 . Then the composition is quartic (fourth degree), not quadratic: 𝑓 (𝑔(π‘₯)) = 𝑓 (π‘₯2 ) = (π‘₯2 )2 = π‘₯4 . 93. True. If we factor and simplify the rational expression, we see that 𝑓 (π‘₯) =

5π‘₯(π‘₯ + 1)(π‘₯ βˆ’ 1) = 5π‘₯ βˆ’ 5, for π‘₯ β‰  βˆ’1, 0. π‘₯(π‘₯ + 1)

Hence, over π‘₯ > 0 the graph of the 𝑓 is the same at the graph of the linear function 𝑦 = 5π‘₯ βˆ’ 5. 94. (a), (c), (d), (e), (b). Notice that 𝑓 (π‘₯) and β„Ž(π‘₯) are decreasing functions, with 𝑓 (π‘₯) being negative. Power functions grow slower than exponential growth functions, so π‘˜(π‘₯) is next. Now order the remaining exponential functions, where functions with larger bases grow faster.

Additional Problems (online only) 95. (a) (I) For linear functions we have 𝑓 (π‘₯ + 2) βˆ’ 𝑓 (π‘₯) = 𝑏 + π‘š(π‘₯ + 2) βˆ’ (𝑏 + π‘šπ‘₯) = 2π‘š. The difference is constant, because it does not depend on π‘₯. (b) (III) For exponential functions we have 𝑓 (π‘₯ + 2) π‘Žπ‘’π‘˜(π‘₯+2) = 𝑓 (π‘₯) π‘Žπ‘’π‘˜π‘₯ π‘Žπ‘’π‘˜π‘₯ 𝑒2π‘˜ = = 𝑒2π‘˜ . π‘Žπ‘’π‘˜π‘₯ The quotient is constant, because it does not depend on π‘₯. (c) (IV) For power functions we have 𝑓 (2π‘₯) π‘Ž(2π‘₯)𝑛 = 𝑓 (π‘₯) π‘Žπ‘₯𝑛 π‘Ž2𝑛 π‘₯𝑛 = = 2𝑛 . π‘Žπ‘₯𝑛 The quotient is constant, because it does not depend on π‘₯. (d) (II) For logarithmic functions we have 𝑓 (2π‘₯) βˆ’ 𝑓 (π‘₯) = (π‘Ž + 𝑏 ln(2π‘₯)) βˆ’ (π‘Ž + 𝑏 ln π‘₯) = (π‘Ž + 𝑏 ln 2 + 𝑏 ln π‘₯) βˆ’ (π‘Ž + 𝑏 ln π‘₯) = 𝑏 ln 2. The difference is constant, because it does not depend on π‘₯.


80

Chapter One /SOLUTIONS

96. Properties of logs give

ln(π‘˜π‘₯𝑝 ) = ln π‘˜ + ln π‘₯𝑝 = ln π‘˜ + 𝑝 ln π‘₯.

Therefore 𝑝

𝑝

ln(π‘˜π‘₯2 ) βˆ’ ln(π‘˜π‘₯1 ) ln 𝑓 (π‘₯2 ) βˆ’ ln 𝑓 (π‘₯1 ) = ln π‘₯2 βˆ’ ln π‘₯1 ln π‘₯2 βˆ’ ln π‘₯1 ln π‘˜ + 𝑝 ln π‘₯2 βˆ’ ln π‘˜ βˆ’ 𝑝 ln π‘₯1 = ln π‘₯2 βˆ’ ln π‘₯1 𝑝(ln π‘₯2 βˆ’ ln π‘₯1 ) = = 𝑝. ln π‘₯2 βˆ’ ln π‘₯1

Solutions for Section 1.7 EXERCISES 1. (a) The function 𝑓 has jumps in the graph at π‘₯ = βˆ’1 and at π‘₯ = 1. Therefore, 𝑓 is not continuous at π‘₯ = βˆ’1 and at π‘₯ = 1. (b) The domain of 𝑓 is βˆ’3 ≀ π‘₯ ≀ 3, and by part (a), we know that 𝑓 is not continuous at π‘₯ = βˆ’1 and at π‘₯ = 1. Therefore, 𝑓 is continuous on βˆ’3 < π‘₯ < βˆ’1, βˆ’1 < π‘₯ < 1, and 1 < π‘₯ < 3. 2. (a) The function 𝑓 has a break in the graph at π‘₯ = 1 and jumps in the graph at π‘₯ = 2 and at π‘₯ = 4. Therefore, 𝑓 is not continuous at π‘₯ = 1, 2, and 4. (b) The domain of 𝑓 is 0 ≀ π‘₯ ≀ 6, and by part (a), we know that 𝑓 is not continuous at π‘₯ = 1, 2 and at 4. Therefore, 𝑓 is continuous on 0 < π‘₯ < 1, 1 < π‘₯ < 2, 2 < π‘₯ < 4, and 4 < π‘₯ < 6. 3. (a) As π‘₯ approaches βˆ’3 from either side, the values of 𝑓 (π‘₯) get closer and closer to 1, so the limit appears to be about 1. (b) As π‘₯ approaches βˆ’2 from either side, the values of 𝑓 (π‘₯) get closer and closer to 2, so the limit appears to be about 2. (c) As π‘₯ approaches βˆ’1, the values of 𝑓 (π‘₯) get closer and closer to 3 on one side of π‘₯ = βˆ’1 and get closer and closer to 2 on the other side of π‘₯ = βˆ’1. Thus the limit does not exist. (d) As π‘₯ approaches 0 from either side, the values of 𝑓 (π‘₯) get closer and closer to 1, so the limit appears to be about 1. (e) As π‘₯ approaches 1 from either side, the values of 𝑓 (π‘₯) get closer and closer to 0, so the limit appears to be about 0. (f) As π‘₯ approaches 3 from either side, the values of 𝑓 (π‘₯) get closer and closer to 2. (Recall that to find a limit, we are interested in what happens to the function near π‘₯ but not at π‘₯.) The limit appears to be about 2. 4. (a) Since the graph has a jump at π‘₯ = βˆ’1, 𝑓 (π‘₯) is not continuous at π‘₯ = βˆ’1. Since the graph has a hole at π‘₯ = 2, 𝑓 (π‘₯) is not continuous at π‘₯ = 2. (b) As π‘₯ approaches βˆ’1 from either side, the values of 𝑓 (π‘₯) get closer and closer to 2 on one side of π‘₯ = βˆ’1 and get closer and closer to 5 on the other side of π‘₯ = βˆ’1. Thus lim 𝑓 (π‘₯) does not exist. As π‘₯ approaches 2 from either side, π‘₯β†’βˆ’1

the values of 𝑓 (π‘₯) get closer and closer to βˆ’3, so the limit appears to be about βˆ’3. 5. (a) Since the graph has a hole at π‘₯ = βˆ’2, 𝑓 (π‘₯) is not continuous at π‘₯ = βˆ’2. Since the graph has an asymptote at π‘₯ = 3, 𝑓 (π‘₯) is not continuous at π‘₯ = 3. (b) As π‘₯ approaches βˆ’2 from either side, the values of 𝑓 (π‘₯) get closer and closer to βˆ’3, so the limit appears to be about βˆ’3. As π‘₯ approaches 3 from either side, the values of 𝑓 (π‘₯) approach ∞. Thus lim 𝑓 (π‘₯) does not exist. π‘₯β†’3

6. Values of 𝑓 (π‘₯) appear to approach 2 as π‘₯ gets close to 0 from both sides, so lim 𝑓 (π‘₯) appears to be 2. π‘₯β†’0

We do not know for sure the limit is 2 because for values of π‘₯ close to 0 different from those in the table, the values of 𝑓 (π‘₯) might not approach 2. For example, they might not approach a limit at all, or they might approach, for example, 2.00001 or 1.9999. 7. Values of 𝑔(𝑑) appear to approach 1 as 𝑑 gets close to 3 from both sides, so lim 𝑔(𝑑) appears to be 1. 𝑑→3

We do not know for sure the limit is 1 because for values of 𝑑 close to 3 different from those in the table, the values of 𝑔(𝑑) might not approach 1. For example, they might not approach a limit at all, or they might approach, for example, 1.00001 or 0.9999. 8. (a) Substituting π‘₯-values into 𝑓 (π‘₯) gives: π‘₯

βˆ’0.1

βˆ’0.01

0.01

0.1

𝑓 (π‘₯)

4.794

4.998

4.998

4.794


1.7 SOLUTIONS

81

(b) Since the values of 𝑓 (π‘₯) appear to get closer and closer to 5 as π‘₯ gets closer and closer to 0, we estimate lim π‘₯β†’0

sin(5π‘₯) = 5. π‘₯

sin(5π‘₯) is undefined at π‘₯ = 0. π‘₯ 9. (a) Substituting π‘₯-values into 𝑓 (π‘₯) gives: Notice that 𝑓 (π‘₯) =

π‘₯

βˆ’0.1

βˆ’0.01

0.01

0.1

𝑓 (π‘₯)

2.592

2.955

3.045

3.499

(b) Since the values of 𝑓 (π‘₯) appear to get closer and closer to 3 as π‘₯ gets closer and closer to 0, we estimate lim π‘₯β†’0

𝑒3π‘₯ βˆ’ 1 = 3. π‘₯

𝑒3π‘₯ βˆ’ 1 is undefined at π‘₯ = 0. π‘₯ 10. We evaluate 𝑓 (π‘₯) = 5 + ln π‘₯ for values of π‘₯ closer and closer to 1. Notice that 𝑓 (π‘₯) =

π‘₯

0.9

0.99

0.999

1.001

1.01

1.1

5 + ln π‘₯

4.895

4.990

4.999

5.001

5.010

5.095

From the table, we see that 𝑓 (π‘₯) gets closer and closer to 5, so we estimate lim(5 + ln π‘₯) = 5. π‘₯β†’1

11. Yes, because π‘₯ βˆ’ 2 is not zero on this interval. 12. No, because π‘₯ βˆ’ 2 = 0 at π‘₯ = 2. 13. Yes, because 2π‘₯ βˆ’ 5 is positive for 3 ≀ π‘₯ ≀ 4. 14. No, because 2π‘₯ + π‘₯βˆ’1 is undefined at π‘₯ = 0. 15. No, because cos(πœ‹βˆ•2) = 0. 16. Yes, because cos πœƒ is not zero on this interval. 17. (a) At π‘₯ = 1, on the line 𝑦 = π‘₯, we have 𝑦 = 1. At π‘₯ = 1, on the parabola 𝑦 = π‘₯2 , we have 𝑦 = 1. Thus, 𝑓 (π‘₯) is continuous. See Figure 1.87. (b) At π‘₯ = 3, on the line 𝑦 = π‘₯, we have 𝑦 = 3. At π‘₯ = 3, on the parabola 𝑦 = π‘₯2 , we have 𝑦 = 9. Thus, 𝑔(π‘₯) is not continuous. See Figure 1.88. 𝑦

𝑦

𝑔(π‘₯)

𝑓 (π‘₯)

1

Figure 1.87

π‘₯

3

π‘₯

Figure 1.88

18. (a) Since the graph of 𝑓 is comprised of portions of either linear or quadratic functions, 𝑓 is continuous everywhere except possibly at π‘₯ = 3 and π‘₯ = 5, where the formula for the function 𝑓 changes. Since the graph of 4 βˆ’ π‘₯ goes through the point (3, 1) but the graph of π‘₯2 βˆ’ 8π‘₯ + 17 goes through the point (3, 2), there is a jump in the graph of 𝑓 at π‘₯ = 3, meaning that 𝑓 is not continuous at π‘₯ = 3. On the other hand, the graph of π‘₯2 βˆ’ 8π‘₯ + 17 and 12 βˆ’ 2π‘₯ both go through the point (5, 2), so 𝑓 is continuous at π‘₯ = 5. Thus, π‘₯ = 3 is the only value of π‘₯ at which 𝑓 is not continuous. (b) By part (a), we know that 𝑓 is not continuous at π‘₯ = 3. Therefore, 𝑓 is continuous on 0 < π‘₯ < 3 and 3 < π‘₯ < 6.


82

Chapter One /SOLUTIONS

19. We have that 𝑓 (0) = βˆ’1 < 0 and 𝑓 (1) = 1 > 0 and that 𝑓 is continuous. Thus, by the Intermediate Value Theorem applied to π‘˜ = 0, there is a number 𝑐 in [0, 1] such that 𝑓 (𝑐) = π‘˜ = 0. 20. We have that 𝑓 (0) = 1 > 0 and 𝑓 (1) = 𝑒 βˆ’ 3 < 0 and that 𝑓 is continuous. Thus, by the Intermediate Value Theorem applied to π‘˜ = 0, there is a number 𝑐 in [0, 1] such that 𝑓 (𝑐) = π‘˜ = 0. 21. We have that 𝑓 (0) = βˆ’1 < 0 and 𝑓 (1) = 1 βˆ’ cos 1 > 0 and that 𝑓 is continuous. Thus, by the Intermediate Value Theorem applied to π‘˜ = 0, there is a number 𝑐 in [0, 1] such that 𝑓 (𝑐) = π‘˜ = 0. 22. Since 𝑓 is not continuous at π‘₯ = 0, we consider instead the smaller interval [0.01, 1]. We have that 𝑓 (0.01) = 20.01 βˆ’100 < 0 and 𝑓 (1) = 2 βˆ’ 1βˆ•1 = 1 > 0 and that 𝑓 is continuous. Thus, by the Intermediate Value Theorem applied to π‘˜ = 0, there is a number 𝑐 in [0.01, 1], and hence in [0, 1], such that 𝑓 (𝑐) = π‘˜ = 0. π‘₯2 βˆ’ 4 at π‘₯ = 2 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have 23. Evaluating π‘₯βˆ’2 (π‘₯ + 2)(π‘₯ βˆ’ 2) π‘₯2 βˆ’ 4 = . π‘₯βˆ’2 π‘₯βˆ’2 Since π‘₯ β‰  2 in the limit, we can cancel the common factor π‘₯ βˆ’ 2 to see lim π‘₯β†’2

24. Evaluating

(π‘₯ + 2)(π‘₯ βˆ’ 2) π‘₯2 βˆ’ 4 = lim = lim(π‘₯ + 2) = 4. π‘₯β†’2 π‘₯β†’2 π‘₯βˆ’2 π‘₯βˆ’2

π‘₯2 βˆ’ 9 at π‘₯ = βˆ’3 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯+3 (π‘₯ + 3)(π‘₯ βˆ’ 3) π‘₯2 βˆ’ 9 = . π‘₯+3 π‘₯+3

Since π‘₯ β‰  βˆ’3 in the limit, we can cancel the common factor π‘₯ + 3 to see lim

π‘₯β†’βˆ’3

25. Evaluating

(π‘₯ + 3)(π‘₯ βˆ’ 3) π‘₯2 βˆ’ 9 = lim = lim (π‘₯ βˆ’ 3) = βˆ’6. π‘₯β†’βˆ’3 π‘₯β†’βˆ’3 π‘₯+3 π‘₯+3

π‘₯2 + 4π‘₯ βˆ’ 5 at π‘₯ = 1 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯βˆ’1 (π‘₯ + 5)(π‘₯ βˆ’ 1) π‘₯2 + 4π‘₯ βˆ’ 5 = . π‘₯βˆ’1 π‘₯βˆ’1

Since π‘₯ β‰  1 in the limit, we can cancel the common factor π‘₯ βˆ’ 1 to see lim π‘₯β†’1

26. Evaluating

(π‘₯ + 5)(π‘₯ βˆ’ 1) π‘₯2 + 4π‘₯ βˆ’ 5 = lim = lim(π‘₯ + 5) = 6. π‘₯β†’1 π‘₯β†’1 π‘₯βˆ’1 π‘₯βˆ’1

π‘₯2 βˆ’ 4π‘₯ + 3 at π‘₯ = 1 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯2 + 3π‘₯ βˆ’ 4 (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3) π‘₯2 βˆ’ 4π‘₯ + 3 = . (π‘₯ + 4)(π‘₯ βˆ’ 1) π‘₯2 + 3π‘₯ βˆ’ 4

Since π‘₯ β‰  1 in the limit, we can cancel the common factor π‘₯ βˆ’ 1 to see lim

π‘₯2 βˆ’ 4π‘₯ + 3

π‘₯β†’1 π‘₯2 + 3π‘₯ βˆ’ 4

= lim

(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 3)

π‘₯β†’1 (π‘₯ + 4)(π‘₯ βˆ’ 1)

= lim

π‘₯βˆ’3

π‘₯β†’1 π‘₯ + 4

=

βˆ’2 . 5

π‘₯2 + 4 is continuous everywhere on its domain (that is, at every point except π‘₯ = βˆ’8.) In particular, it is π‘₯+8 continuous at π‘₯ = 1 so we find the limit by evaluating the expression at π‘₯ = 1. We have

27. The expression

5 π‘₯2 + 4 = . π‘₯β†’1 π‘₯ + 8 9

lim


1.7 SOLUTIONS

83

28. Evaluating the expression at β„Ž = 0, we arrive at 0βˆ•0. Rewriting the expression using algebra gives lim

β„Žβ†’0

(5 + β„Ž)2 βˆ’ 52 (25 + 10β„Ž + β„Ž2 ) βˆ’ 25 = lim β„Žβ†’0 β„Ž β„Ž 10β„Ž + β„Ž2 = lim β„Žβ†’0 β„Ž β„Ž(10 + β„Ž) = lim β„Žβ†’0 β„Ž and since β„Ž β‰  0, canceling the common factor of β„Ž, we have = lim(10 + β„Ž) β„Žβ†’0

= 10.

29. Since π‘˜π‘₯ + 10 is continuous at π‘₯ = 5, the limit can be found by substituting π‘₯ = 5. Thus, π‘˜(5) + 10 = 20 π‘˜ = 2. 30. Since (π‘₯ + 6)(π‘₯ βˆ’ π‘˜)βˆ•(π‘₯2 + π‘₯) is continuous at π‘₯ = 2, the limit can be found by substituting π‘₯ = 2. Thus, (2 + 6)(2 βˆ’ π‘˜) =4 22 + 2 π‘˜ = βˆ’1. 31. The value of 𝑦 on the line 𝑦 = π‘˜π‘₯ at π‘₯ = 3 is 𝑦 = 3π‘˜. To make 𝑓 (π‘₯) continuous, we need 3π‘˜ = 5

so

π‘˜=

5 . 3

See Figure 1.89. 𝑦

𝑓 (π‘₯)

5

6 𝑦=5

I

𝑦 = (5βˆ•3)π‘₯ 3

π‘₯

Figure 1.89

32. For any value of π‘˜, the function is continuous at every point except π‘₯ = 2. We choose π‘˜ to make the function continuous at π‘₯ = 2. Since 3π‘₯2 takes the value 3(22 ) = 12 at π‘₯ = 2, we choose π‘˜ so that the graph of π‘˜π‘₯ goes through the point (2, 12). Thus π‘˜ = 6. 33. For any value of π‘˜, the function is continuous at every point except π‘₯ = 1. We choose π‘˜ to make the function continuous at π‘₯ = 1. Since π‘₯ + 3 takes the value 1 + 3 = 4 at π‘₯ = 1, we choose π‘˜ so that the graph of π‘˜π‘₯ goes through the point (1, 4). Thus π‘˜ = 4. 34. If the graphs of 𝑦 = 𝑑 + π‘˜ and 𝑦 = π‘˜π‘‘ meet at 𝑑 = 5, we have 5 + π‘˜ = 5π‘˜ π‘˜ = 5βˆ•4. See Figure 1.90.


84

Chapter One /SOLUTIONS 𝑦 𝑦 = (5βˆ•4)𝑑 𝑔(𝑑) 𝑦 = (5βˆ•4) + 𝑑

5 4

5

10

𝑑

Figure 1.90

PROBLEMS 35. (a) Even if the car stops to refuel, the amount of fuel in the tank changes smoothly, so the fuel in the tank is a continuous function; the quantity of fuel cannot suddenly change from one value to another. (b) Whenever a student joins or leaves the class the number jumps up or down immediately by 1 so this is not a continuous function, unless the enrollment does not change at all. (c) Whenever the oldest person dies the value of the function jumps down to the age of the next oldest person, so this is not a continuous function. 36. The voltage 𝑓 (𝑑) is graphed in Figure 1.91. 12

6

time (seconds)

7

Figure 1.91: Voltage change from 6V to 12V Using formulas, the voltage, 𝑓 (𝑑), is represented by { 𝑓 (𝑑) =

6,

0<𝑑≀7

12,

7<𝑑

Although a real physical voltage is continuous, the voltage in this circuit is well-approximated by the function 𝑓 (𝑑), which is not continuous on any interval around 7 seconds. 37. (a) The function 𝑓 has a jump in the graph at 𝑑 = 5 so it is not continuous. The discontinuity at 𝑑 = 5 occurs because the speed of the rock suddenly drops to zero when it hits the ground. (b) The stone starts at the top of the cliff and its height decreases over time until 𝑑 = 5 when it hits the ground. For 5 ≀ 𝑑 ≀ 7, we have β„Ž = 0 since the stone is on the ground. Therefore Figure 1.92 is a possible graph. The function 𝑔 is continuous because there is no sudden change in the height of the stone. β„Ž

𝑔(𝑑)

5

Figure 1.92

7

𝑑


1.7 SOLUTIONS

85

38. (a) For 0 ≀ 𝑑 ≀ 2, the car is accelerating, so 𝑓 is increasing. For 2 ≀ 𝑑 ≀ 3, the speed of the car is constant, so 𝑓 is constant. Finally, at 𝑑 = 3, the speed of the car drops to zero when it hits the barrier. A possible graph of 𝑓 is shown in Figure 1.93. 𝑣

1

2

3

4

𝑑

Figure 1.93 (b) No, 𝑓 is not continuous because the speed of the car suddenly drops when it hits the barrier, resulting in a jump in the graph of 𝑓 at 𝑑 = 3 seconds. 39. The graph of 𝑔 suggests that 𝑔 is not continuous on any interval containing πœƒ = 0, since 𝑔(0) = 1βˆ•2. 40. For π‘₯ > 0, we have |π‘₯| = π‘₯, so 𝑓 (π‘₯) = 1. For π‘₯ < 0, we have |π‘₯| = βˆ’π‘₯, so 𝑓 (π‘₯) = βˆ’1. Thus, the function is given by { 1 π‘₯>0 𝑓 (π‘₯) = 0 π‘₯=0 βˆ’1 π‘₯ < 0 , so 𝑓 is not continuous on any interval containing π‘₯ = 0. |π‘₯| does not exist. See Figure 1.94. 41. The break in the graph at π‘₯ = 0 suggests that lim π‘₯β†’0 π‘₯ 1

|π‘₯| π‘₯

βˆ’1

1

π‘₯

βˆ’1

Figure 1.94 42. For βˆ’1 ≀ π‘₯ ≀ 1, βˆ’ 1 ≀ 𝑦 ≀ 1, the graph of 𝑦 = π‘₯ ln |π‘₯| is in Figure 1.95. The graph suggests that lim π‘₯ ln |π‘₯| = 0. π‘₯β†’0

𝑦 1 𝑦 = π‘₯ ln |π‘₯|

βˆ’1

1

βˆ’1

Figure 1.95

π‘₯


86

Chapter One /SOLUTIONS

43. For βˆ’0.5 ≀ πœƒ ≀ 0.5, 0 ≀ 𝑦 ≀ 3, the graph of 𝑦 =

sin (2πœƒ) is shown in Figure 1.96. The graph suggests that πœƒ sin (2πœƒ) lim = 2. πœƒβ†’0 πœƒ 𝑦

𝑦 = sin(2πœƒ) πœƒ

0

0.5

2 1

βˆ’0.5

πœƒ

Figure 1.96 sin πœƒ 44. For βˆ’90β—¦ ≀ πœƒ ≀ 90β—¦ , 0 ≀ 𝑦 ≀ 0.02, the graph of 𝑦 = is shown in Figure 1.97. By tracing along the curve, we see πœƒ that in degrees, sin πœƒ = 0.01745 … . lim πœƒβ†’0 πœƒ sin πœƒ πœƒ

0.02 0.01

βˆ’90

0

90

πœƒ (degree)

Figure 1.97

45. A graph of 𝑦 = estimate that

π‘’β„Ž βˆ’ 1 in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and 0 ≀ 𝑦 ≀ 3 appears to indicate 𝑦 β†’ 1 as β„Ž β†’ 0. We β„Ž π‘’β„Ž βˆ’ 1 = 1. β„Žβ†’0 β„Ž lim

46. A graph of 𝑦 = estimate that

𝑒5β„Ž βˆ’ 1 in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and 0 ≀ 𝑦 ≀ 6 appears to indicate 𝑦 β†’ 5 as β„Ž β†’ 0. We β„Ž lim

β„Žβ†’0

𝑒5β„Ž βˆ’ 1 = 5. β„Ž

2β„Ž βˆ’ 1 47. A graph of 𝑦 = in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and 0 ≀ 𝑦 ≀ 1 appears to indicate 𝑦 β†’ 0.7 as β„Ž β†’ 0. By β„Ž zooming in on the graph, we can estimate the limit more accurately. Therefore, we estimate that lim

β„Žβ†’0

2β„Ž βˆ’ 1 = 0.693. β„Ž

cos(3β„Ž) βˆ’ 1 in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and βˆ’1 ≀ 𝑦 ≀ 1 appears to indicate 𝑦 β†’ 0 as β„Ž β†’ 0. 48. A graph of 𝑦 = β„Ž Therefore, we estimate that cos(3β„Ž) βˆ’ 1 = 0. lim β„Žβ†’0 β„Ž


1.7 SOLUTIONS

87

49. Let 𝑓 (π‘₯) = (2π‘₯2 βˆ’ 32)βˆ•(π‘₯ + 4). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 4 by putting in π‘₯-values closer and closer to π‘₯ = 4. In Table 1.8 the values of 𝑓 (π‘₯) appear to get closer and closer to 0 as π‘₯ gets closer to 4, so we estimate 2π‘₯2 βˆ’ 32 = 0. π‘₯β†’4 π‘₯+4

lim

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.98 suggests that lim π‘₯β†’4

2π‘₯2 βˆ’ 32 = 0. π‘₯+4

Since 𝑓 (π‘₯) is continuous at π‘₯ = 4, we can also find the limit exactly by substituting π‘₯ = 4. This gives 2 β‹… 42 βˆ’ 32 2π‘₯2 βˆ’ 32 = = 0. π‘₯β†’4 π‘₯+4 4+4

lim Table 1.8 π‘₯

3.9

3.99

3.999

4.001

4.01

4.1

𝑓 (π‘₯)

βˆ’0.2

βˆ’0.02

βˆ’0.002

0.002

0.02

0.2

1 0.5 0

3.5

βˆ’0.5

4

4.5

5

π‘₯

βˆ’1

Figure 1.98 50. Let 𝑓 (π‘₯) = (2π‘₯2 βˆ’ 32)βˆ•(π‘₯ + 4). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to βˆ’4 by putting in π‘₯-values closer and closer to π‘₯ = βˆ’4. In Table 1.9, the values of 𝑓 (π‘₯) appear to get closer and closer to βˆ’16 as π‘₯ gets closer to βˆ’4, so we estimate lim

π‘₯β†’βˆ’4

2π‘₯2 βˆ’ 32 = βˆ’16. π‘₯+4

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.99 suggests that 2π‘₯2 βˆ’ 32 = βˆ’16. π‘₯β†’βˆ’4 π‘₯ + 4 lim

We can also use algebra to find the limit exactly. We have 2(π‘₯ + 4)(π‘₯ βˆ’ 4) 2π‘₯2 βˆ’ 32 = . π‘₯+4 π‘₯+4 Since π‘₯ β‰  βˆ’4 in the limit, we can cancel the common factor π‘₯ + 4 to see 2(π‘₯ + 4)(π‘₯ βˆ’ 4) 2π‘₯2 βˆ’ 32 = lim = lim 2(π‘₯ βˆ’ 4) = βˆ’16. π‘₯β†’βˆ’4 π‘₯ + 4 π‘₯β†’βˆ’4 π‘₯β†’βˆ’4 π‘₯+4 lim

Table 1.9 π‘₯

βˆ’4.1

βˆ’4.01

βˆ’4.001

βˆ’3.999

βˆ’3.99

βˆ’3.9

𝑓 (π‘₯)

βˆ’16.2

βˆ’16.02

βˆ’16.002

βˆ’15.998

βˆ’15.98

βˆ’15.8

βˆ’5

βˆ’4.5

βˆ’4

βˆ’3.5

π‘₯ βˆ’15

(βˆ’4, βˆ’16)

βˆ’16 βˆ’17 βˆ’18

Figure 1.99


88

Chapter One /SOLUTIONS

51. Let 𝑓 (π‘₯) = (3π‘₯ βˆ’ 1)βˆ•(sin π‘₯). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 0 by putting in π‘₯-values closer and closer to π‘₯ = 0. In Table 1.10, the values of 𝑓 (π‘₯) appear to get closer and closer to 1.099 as π‘₯ gets closer to 0, so we estimate lim π‘₯β†’0

3π‘₯ βˆ’ 1 = 1.099. sin π‘₯

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.100 suggests that lim π‘₯β†’0

3π‘₯ βˆ’ 1 = 1.099. sin π‘₯

There are no direct purely algebraic manipulations we can perform to calculate this limit exactly. Table 1.10 π‘₯

βˆ’0.1

βˆ’0.01

βˆ’0.001

βˆ’0.0001

0.0001

0.001

0.01

0.1

𝑓 (π‘₯)

1.042

1.093

1.098

1.099

1.099

1.099

1.105

1.163

1.5 (0, 1.099)

1 0.5 βˆ’0.5 βˆ’0.25

0

0.25

π‘₯

0.5

Figure 1.100 √ 52. Let 𝑓 (π‘₯) = ( π‘₯ βˆ’ 2)βˆ•(π‘₯ βˆ’ 4). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 4 by putting in π‘₯-values closer and closer to π‘₯ = 4. In Table 1.11, the values of 𝑓 (π‘₯) appear to get closer and closer to 0.25 as π‘₯ gets closer to 4, so we estimate √ π‘₯βˆ’2 = 0.25. lim π‘₯β†’4 π‘₯ βˆ’ 4 Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.101 suggests that √ π‘₯βˆ’2 lim = 0.25. π‘₯β†’4 π‘₯ βˆ’ 4 We can also use algebra to find the limit exactly. We have √ √ π‘₯βˆ’2 π‘₯βˆ’2 . = √ √ π‘₯βˆ’4 ( π‘₯ βˆ’ 2)( π‘₯ + 2) √ Since π‘₯ β‰  4 in the limit, we can cancel the common factor π‘₯ βˆ’ 2 to see √ √ π‘₯βˆ’2 π‘₯βˆ’2 1 1 = lim √ = = 0.25. lim = lim √ √ π‘₯β†’4 π‘₯ βˆ’ 4 π‘₯β†’4 π‘₯β†’4 4 ( π‘₯ βˆ’ 2)( π‘₯ + 2) π‘₯+2 Table 1.11 π‘₯

3.9

3.99

3.999

4.001

4.01

4.1

𝑓 (π‘₯)

0.2516

0.2502

0.25002

0.24998

0.2498

0.2485

0.5 (4, 0.25)

0.25

3

4

Figure 1.101

5

π‘₯


1.7 SOLUTIONS

89

53. Let 𝑓 (π‘₯) = (π‘₯4 βˆ’ π‘₯2 )βˆ•(π‘₯ + 1). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 1 by putting in π‘₯-values closer and closer to π‘₯ = βˆ’1. In Table 1.12, the values of 𝑓 (π‘₯) appear to get closer and closer to βˆ’2 as π‘₯ gets closer to βˆ’1, so we estimate π‘₯ 4 βˆ’ π‘₯2 = βˆ’2. π‘₯β†’βˆ’1 π‘₯ + 1 lim

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.102 suggests that lim

π‘₯β†’βˆ’1

π‘₯ 4 βˆ’ π‘₯2 = βˆ’2. π‘₯+1

We can also use algebra to find the limit exactly. We have π‘₯2 (π‘₯2 βˆ’ 1) π‘₯2 (π‘₯ βˆ’ 1)(π‘₯ + 1) π‘₯4 βˆ’ π‘₯ 2 = = . π‘₯+1 π‘₯+1 π‘₯+1 Since π‘₯ β‰  βˆ’1 in the limit, we can cancel the common factor π‘₯ + 1 to see π‘₯2 (π‘₯ βˆ’ 1)(π‘₯ + 1) π‘₯ 4 βˆ’ π‘₯2 = lim = lim π‘₯2 (π‘₯ βˆ’ 1) = βˆ’2. π‘₯β†’βˆ’1 π‘₯ + 1 π‘₯β†’βˆ’1 π‘₯β†’βˆ’1 π‘₯+1 lim

Table 1.12 π‘₯

βˆ’1.1

βˆ’1.01

βˆ’1.001

βˆ’0.999

βˆ’0.99

βˆ’0.9

𝑓 (π‘₯)

βˆ’2.541

βˆ’2.05

βˆ’2.005

βˆ’1.995

βˆ’1.95

βˆ’1.539

βˆ’1.5

βˆ’1

βˆ’0.5

2 π‘₯ βˆ’2

(βˆ’1 βˆ’ 2)

βˆ’4 βˆ’6

Figure 1.102 54. Let 𝑓 (π‘₯) = (16 βˆ’ 8π‘₯)βˆ•(2π‘₯ βˆ’ 4). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 2 by putting in π‘₯-values closer and closer to π‘₯ = 2. In Table 1.13, the values of 𝑓 (π‘₯) appear to get closer and closer to βˆ’2.885 as π‘₯ gets closer and closer to 2, so we estimate 16 βˆ’ 8π‘₯ = βˆ’2.885. lim π‘₯ π‘₯β†’2 2 βˆ’ 4 Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.103 suggests that lim π‘₯β†’2

16 βˆ’ 8π‘₯ = βˆ’2.885. 2π‘₯ βˆ’ 4

There are no direct purely algebraic manipulations we can perform to calculate this limit exactly. Table 1.13 π‘₯

1.9

1.99

1.999

1.9999

2.0001

2.001

2.01

2.1

𝑓 (π‘₯)

βˆ’2.987

βˆ’2.895

βˆ’2.886

βˆ’2.885

βˆ’2.885

βˆ’2.884

βˆ’2.875

βˆ’2.787

0

1

2

βˆ’3

3

π‘₯

(2, βˆ’2.885)

βˆ’6

Figure 1.103


90

Chapter One /SOLUTIONS

55. Let 𝑓 (π‘₯) = (1 βˆ’ 3π‘₯ )βˆ•(𝑒π‘₯ βˆ’ 1). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 0 by putting in π‘₯-values closer and closer to π‘₯ = 0. In Table 1.14, the values of 𝑓 (π‘₯) appear to get closer and closer to βˆ’1.099 as π‘₯ gets closer to 0, so we estimate 1 βˆ’ 3π‘₯ = βˆ’1.099. π‘₯β†’0 𝑒π‘₯ βˆ’ 1

lim

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.104 suggests that lim

1 βˆ’ 3π‘₯

π‘₯β†’0 𝑒π‘₯ βˆ’ 1

= βˆ’1.099.

There are no direct purely algebraic manipulations we can perform to calculate this limit exactly. Table 1.14 π‘₯

βˆ’0.1

βˆ’0.01

βˆ’0.001

0.001

0.01

0.1

𝑓 (π‘₯)

βˆ’1.093

βˆ’1.098

βˆ’1.099

βˆ’1.099

βˆ’1.099

βˆ’1.104

βˆ’1

βˆ’0.5

0.5

π‘₯

1

βˆ’1 (0, βˆ’1.099) βˆ’2

Figure 1.104 56. Let 𝑓 (π‘₯) = (4π‘₯ βˆ’ 16)βˆ•(2π‘₯ βˆ’ 4). We can estimate the limit of 𝑓 (π‘₯) as π‘₯ goes to 2 by putting in π‘₯-values closer and closer to π‘₯ = 2. In Table 1.15, the values of 𝑓 (π‘₯) appear to get closer and closer to 8 as π‘₯ gets closer to 2, so we estimate lim π‘₯β†’2

4π‘₯ βˆ’ 16 = 8. 2π‘₯ βˆ’ 4

Alternatively, we can use the graph of 𝑓 (π‘₯) to estimate the limit. Figure 1.105 suggests that 4π‘₯ βˆ’ 16 = 8. π‘₯β†’2 2π‘₯ βˆ’ 4

lim

We can also use algebra to find the limit exactly. We have (2π‘₯ )2 βˆ’ 16 (2π‘₯ βˆ’ 4)(2π‘₯ + 4) 4π‘₯ βˆ’ 16 = = . 2π‘₯ βˆ’ 4 2π‘₯ βˆ’ 4 2π‘₯ βˆ’ 4 Since π‘₯ β‰  2 in the limit, we can cancel the common factor 2π‘₯ βˆ’ 4 to see (2π‘₯ βˆ’ 4)(2π‘₯ + 4) 4π‘₯ βˆ’ 16 = lim = lim(2π‘₯ + 4) = 8. π‘₯ π‘₯β†’2 2 βˆ’ 4 π‘₯β†’2 π‘₯β†’2 2π‘₯ βˆ’ 4

lim

Table 1.15 π‘₯

1.9

1.99

1.999

2.001

2.01

2.1

𝑓 (π‘₯)

7.732

7.972

7.997

8.003

8.028

8.287

12 8

(2, 8)

4 0

1

2

Figure 1.105

3

π‘₯


1.7 SOLUTIONS

91

57. At π‘₯ = πœ‹, the curve 𝑦 = π‘˜ cos π‘₯ has 𝑦 = π‘˜ cos πœ‹ = βˆ’π‘˜. At π‘₯ = πœ‹, the line 𝑦 = 12 βˆ’ π‘₯ has 𝑦 = 12 βˆ’ πœ‹. If β„Ž(π‘₯) is continuous, we need βˆ’π‘˜ = 12 βˆ’ πœ‹ π‘˜ = πœ‹ βˆ’ 12. 58. For any value of π‘˜, the function is continuous at every point except π‘₯ = 1. We choose π‘˜ to make the function continuous at π‘₯ = 1. Since π‘˜π‘₯ takes the value π‘˜ β‹… 1 = π‘˜ at π‘₯ = 1, we choose π‘˜ so that the graph of 2π‘˜π‘₯ + 3 goes through the point (1, π‘˜). This gives 2π‘˜ β‹… 1 + 3 = π‘˜ π‘˜ = βˆ’3. 59. For any value of π‘˜, the function is continuous at every point except π‘₯ = πœ‹. We choose π‘˜ to make the function continuous at π‘₯ = πœ‹. Since π‘˜ sin π‘₯ takes the value π‘˜ sin πœ‹ = 0 at π‘₯ = πœ‹, we cannot choose π‘˜ so that the graph of π‘₯ + 4 goes through the point (πœ‹, 0). Thus, this function is discontinuous for all values of π‘˜. 60. For any value of π‘˜, the function is continuous at every point except π‘₯ = 2. We choose π‘˜ to make the function continuous at π‘₯ = 2. Since π‘₯ + 1 takes the value 2 + 1 = 3 at π‘₯ = 2, we choose π‘˜ so that the graph of π‘’π‘˜π‘₯ goes through the point (2, 3). This gives 𝑒2π‘˜ = 3 2π‘˜ = ln 3 ln 3 π‘˜= 2 61. For any value of π‘˜, the function is continuous at every point except π‘₯ = 1. We choose π‘˜ to make the function continuous at π‘₯ = 1. Since sin(π‘˜π‘₯) takes the value sin π‘˜ at π‘₯ = 1, we choose π‘˜ so that the graph of 0.5π‘₯ goes through the point (1, sin π‘˜). This gives sin π‘˜ = 0.5 π‘˜ = sinβˆ’1 0.5 =

πœ‹ . 6

Other solutions are possible. 62. For any value of π‘˜, the function is continuous at every point except π‘₯ = 2. We choose π‘˜ to make the function continuous at π‘₯ = 2. Since ln(π‘˜π‘₯ + 1) takes the value ln(2π‘˜ + 1) at π‘₯ = 2, we choose π‘˜ so that the graph of π‘₯ + 4 goes through the point (2, ln(2π‘˜ + 1)). This gives ln(2π‘˜ + 1) = 2 + 4 = 6 2π‘˜ + 1 = 𝑒6 𝑒6 βˆ’ 1 π‘˜= . 2 63. (a) We see that 𝑓 (π‘₯) has jumps at the points π‘₯ = 1, π‘₯ = 3, and π‘₯ = 5. Therefore, 𝑓 (π‘₯) is discontinuous at π‘₯ = 1, 3, and 5. (b) Observe that, on the intervals 0 ≀ π‘₯ < 1 and 3 < π‘₯ ≀ 5, the function 𝑓 (π‘₯) is positive, so |𝑓 (π‘₯)| = 𝑓 (π‘₯). On the interval 1 ≀ π‘₯ ≀ 3, we have |𝑓 (π‘₯)| = | βˆ’ 2| = 2, and on the interval 5 < π‘₯ ≀ 6, we have |𝑓 (π‘₯)| = | βˆ’ 3| = 3. Using this information, we sketch the graph of |𝑓 (π‘₯)| in Figure 1.106. We see that |𝑓 (π‘₯)| is discontinuous only at π‘₯ = 3, where the graph of |𝑓 (π‘₯)| has a jump.


92

Chapter One /SOLUTIONS |𝑓 (π‘₯)|

3 2 1 1

2

3

4

5

6

π‘₯

Figure 1.106 64. (a) The initial value is when 𝑑 = 0, and we see that 𝑃 (0) = π‘’π‘˜β‹…0 = 𝑒0 = 1000. (b) Since the function is continuous, at 𝑑 = 12, we have π‘’π‘˜π‘‘ = 100 and we solve for π‘˜: 𝑒12π‘˜ = 100 12π‘˜ = ln 100 ln 100 π‘˜= = 0.384. 12 (c) The population is increasing exponentially for 12 months and then becoming constant. 65. The drug first increases linearly for half a second, at the end of which time there is 0.6 ml in the body. Thus, for 0 ≀ 𝑑 ≀ 0.5, the function is linear with slope 0.6βˆ•0.5 = 1.2: 𝑄 = 1.2𝑑

for

0 ≀ 𝑑 ≀ 0.5.

At 𝑑 = 0.5, we have 𝑄 = 0.6. For 𝑑 > 0.5, the quantity decays exponentially at a continuous rate of 0.002, so 𝑄 has the form 0.5 < 𝑑. 𝑄 = π΄π‘’βˆ’0.002𝑑 We choose 𝐴 so that 𝑄 = 0.6 when 𝑑 = 0.5: 0.6 = π΄π‘’βˆ’0.002(0.5) = π΄π‘’βˆ’0.001 𝐴 = 0.6𝑒0.001 . {

Thus 𝑄=

1.2𝑑

0 ≀ 𝑑 ≀ 0.5

0.6𝑒0.001 π‘’βˆ’.002𝑑 0.5 < 𝑑. 66. At π‘₯ = βˆ’1, the function is not defined. Thus, 𝑓 (π‘₯) is not continuous at π‘₯ = βˆ’1. We have (π‘₯ βˆ’ 1)(π‘₯ + 1) π‘₯2 βˆ’ 1 = lim = lim (π‘₯ βˆ’ 1) = βˆ’2. π‘₯β†’βˆ’1 π‘₯β†’βˆ’1 π‘₯+1 π‘₯+1 So if we let 𝑓 (βˆ’1) = βˆ’2, the function is continuous everywhere. lim

π‘₯β†’βˆ’1

67. At π‘₯ = 5, the function is not defined. Thus, 𝑔(π‘₯) is not continuous at π‘₯ = 5. We have (π‘₯ βˆ’ 5)(π‘₯ + 1) π‘₯2 βˆ’ 4π‘₯ βˆ’ 5 = lim = lim(π‘₯ + 1) = 6. π‘₯β†’5 π‘₯β†’5 π‘₯β†’5 π‘₯βˆ’5 π‘₯βˆ’5 So if we let 𝑔(5) = 6, the function is continuous everywhere. lim

68. At 𝑧 = 9, the function is not defined. Thus, 𝑓 (𝑧) is not continuous at 𝑧 = 9. We have lim 𝑧→9

(𝑧 βˆ’ 2)(𝑧 βˆ’ 9) 7 𝑧2 βˆ’ 11𝑧 + 18 π‘§βˆ’2 = lim = lim = . 𝑧→9 𝑧→9 2𝑧 βˆ’ 18 2(𝑧 βˆ’ 9) 2 2

So if we let 𝑓 (9) = 7βˆ•2, the function is continuous everywhere. 69. At 𝑑 = 3 and 𝑑 = βˆ’3, the function is not defined. Thus, π‘ž(𝑑) is not continuous at 𝑑 = Β±3. We have lim 𝑑→3

βˆ’π‘‘(𝑑 βˆ’ 3)(𝑑 + 3) βˆ’π‘‘3 + 9𝑑 = lim = lim βˆ’π‘‘ = βˆ’3. 2 𝑑→3 𝑑→3 (𝑑 βˆ’ 3)(𝑑 + 3) 𝑑 βˆ’9

Similarly, we have

βˆ’π‘‘(𝑑 βˆ’ 3)(𝑑 + 3) βˆ’π‘‘3 + 9𝑑 = lim = lim βˆ’π‘‘ = 3. 2 π‘‘β†’βˆ’3 π‘‘β†’βˆ’3 (𝑑 βˆ’ 3)(𝑑 + 3) 𝑑 βˆ’9 So if we let π‘ž(3) = βˆ’3 and π‘ž(βˆ’3) = 3, the function is continuous everywhere. lim

π‘‘β†’βˆ’3

70. At π‘₯ = 0, the function is not defined. In addition, limπ‘₯β†’0 𝑓 (π‘₯) does not exist. Thus, 𝑓 (π‘₯) is not continuous at π‘₯ = 0.


1.7 SOLUTIONS

93

71. Since limπ‘₯β†’0+ 𝑓 (π‘₯) = 1 and limπ‘₯β†’0βˆ’ 𝑓 (π‘₯) = βˆ’1, we see that limπ‘₯β†’0 𝑓 (π‘₯) does not exist. Thus, 𝑓 (π‘₯) is not continuous at π‘₯=0 72. Since π‘₯βˆ•π‘₯ = 1 for π‘₯ β‰  0, this function 𝑓 (π‘₯) = 1 for all π‘₯. Thus, 𝑓 (π‘₯) is continuous for all π‘₯. 73. Since 2π‘₯βˆ•π‘₯ = 2 for π‘₯ β‰  0, we have limπ‘₯β†’0 𝑓 (π‘₯) = 2, so lim 𝑓 (π‘₯) β‰  𝑓 (0) = 3. π‘₯β†’0

Thus, 𝑓 (π‘₯) is not continuous at π‘₯ = 0. 74.

0.8 0.2

0.4

0.8

1

0.6

0.2

0.4

0.8

1

0.6

0.2

0.4

1

0.6

75. Since polynomials are continuous, and since 𝑝(5) < 0 and 𝑝(10) > 0 and 𝑝(12) < 0, there are two zeros, one between π‘₯ = 5 and π‘₯ = 10, and another between π‘₯ = 10 and π‘₯ = 12. Thus, 𝑝(π‘₯) is a cubic with at least two zeros. If 𝑝(π‘₯) has only two zeros, one would be a double zero (corresponding to a repeated factor). However, since a polynomial does not change sign at a repeated zero, 𝑝(π‘₯) cannot have a double zero and have the signs it does. Thus, 𝑝(π‘₯) has three zeros. The third zero can be greater than 12 or less than 5. See Figures 1.107 and 1.108. 𝑝(π‘₯) π‘₯

π‘₯ 𝑝(π‘₯)

Figure 1.107

Figure 1.108

76. (a) The graphs of 𝑦 = 𝑒π‘₯ and 𝑦 = 4 βˆ’ π‘₯2 cross twice in Figure 1.109. This tells us that the equation 𝑒π‘₯ = 4 βˆ’ π‘₯2 has two solutions. Since 𝑦 = 𝑒π‘₯ increases for all π‘₯ and 𝑦 = 4 βˆ’ π‘₯2 increases for π‘₯ < 0 and decreases for π‘₯ > 0, these are only the two crossing points. 𝑦

𝑦 = 𝑒π‘₯ βˆ’2

2

𝑦 = π‘₯2 βˆ’ 4 π‘₯

Figure 1.109 (b) Values of 𝑓 (π‘₯) are in Table 1.16. One solution is between π‘₯ = βˆ’2 and π‘₯ = βˆ’1; the second solution is between π‘₯ = 1 and π‘₯ = 2. Table 1.16 π‘₯

βˆ’4

βˆ’3

βˆ’2

βˆ’1

0

1

2

3

4

𝑓 (π‘₯)

12.0

5.0

0.1

βˆ’2.6

βˆ’3

βˆ’0.3

7.4

25.1

66.6

77. (a) Since 𝑓 (π‘₯) is not continuous at π‘₯ = 1, it does not satisfy the conditions of the Intermediate Value Theorem. (b) We see that 𝑓 (0) = 𝑒0 = 1 and 𝑓 (2) = 4 + (2 βˆ’ 1)2 = 5. Since 𝑒π‘₯ is increasing between π‘₯ = 0 and π‘₯ = 1, and since 4 + (π‘₯ βˆ’ 1)2 is increasing between π‘₯ = 1 and π‘₯ = 2, any value of π‘˜ between 𝑒1 = 𝑒 and 4 + (1 βˆ’ 1)2 = 4, such as π‘˜ = 3, is a value such that 𝑓 (π‘₯) = π‘˜ has no solution.


94

Chapter One /SOLUTIONS

78. A function 𝑦 = 𝑔(π‘₯) is invertible only if each 𝑦-value corresponds to a unique π‘₯-value. (This condition is called the "horizontal line test" as it tells us that every horizontal line cuts the graph of an invertible function at most once.) We will find a value 𝑦 corresponding to two different π‘₯-values. Since 𝑔(π‘₯) is continuous with 𝑔(0) = 3 and 𝑔(1) = 8, the Intermediate Value Theorem guarantees that between π‘₯ = 0 and π‘₯ = 1, the function 𝑔(π‘₯) takes every value between 3 and 8. We pick any one of the 𝑦-values between 3 and 8 that is also between 8 and 4. We will pick 𝑦 = 6, but it could equally well be 5.5 or 7. By the Intermediate Value Theorem, there exists a number 𝑐 between π‘₯ = 0 and π‘₯ = 1 with 𝑔(𝑐) = 6. Likewise, since 𝑔(π‘₯) is continuous with 𝑔(1) = 8 and 𝑔(2) = 4, the Intermediate Value Theorem guarantees that between π‘₯ = 1 and π‘₯ = 2, the function 𝑔(π‘₯) takes every value between 4 and 8. In particular, there is a number 𝑑 between π‘₯ = 1 and π‘₯ = 2 with 𝑔(𝑑) = 6. This means there are two π‘₯-values, π‘₯ = 𝑐 and π‘₯ = 𝑑, with 𝑐 between 0 and 1 and 𝑑 between 1 and 2, so 𝑐 β‰  𝑑 and 𝑔(𝑐) = 𝑔(𝑑). Thus 𝑔(π‘₯) is not invertible. 79. The answer (see the graph in Figure 1.110) appears to be about 2.7; if we zoom in further, it appears to be about 2.72, which is close to the value of 𝑒 β‰ˆ 2.71828. 𝑦 3.5 3 2.5 2 1.5 1 0.5

𝑦 = (1 + π‘₯)1βˆ•π‘₯

βˆ’0.1

0.1

π‘₯

Figure 1.110

80. We use values of β„Ž approaching, but not equal to, zero. If we let β„Ž = 0.01, 0.001, 0.0001, 0.00001, we calculate the values 2.7048, 2.7169, 2.7181, and 2.7183. If we let β„Ž = βˆ’0.01 βˆ’0.001, βˆ’0.0001, βˆ’0.00001, we get values 2.7320, 2.7196, 2.7184, and 2.7183. These numbers suggest that the limit is the number 𝑒 = 2.71828 …. However, these calculations cannot tell us that the limit is exactly 𝑒; for that a proof is needed. 81. (a) Since sin(π‘›πœ‹) = 0 for 𝑛 = 1, 2, 3, … the sequence of π‘₯-values 1 1 1 , , ,… πœ‹ 2πœ‹ 3πœ‹ works. These π‘₯-values β†’ 0 and are zeroes of 𝑓 (π‘₯). (b) Since sin(π‘›πœ‹βˆ•2) = 1 for 𝑛 = 1, 5, 9 … the sequence of π‘₯-values 2 2 2 , , ,… πœ‹ 5πœ‹ 9πœ‹ works. (c) Since sin(π‘›πœ‹)βˆ•2 = βˆ’1 for 𝑛 = 3, 7, 11, … the sequence of π‘₯-values 2 2 2 , , … 3πœ‹ 7πœ‹ 11πœ‹ works. (d) Any two of these sequences of π‘₯-values show that if the limit were to exist, then it would have to have two (different) values: 0 and 1, or 0 and βˆ’1, or 1 and βˆ’1. Hence, the limit can not exist.

Strengthen Your Understanding 82. The Intermediate Value theorem only makes this guarantee for a continuous function, not for any function. 83. The Intermediate Value Theorem guarantees that for at least one value of π‘₯ between 0 and 2, we have 𝑓 (π‘₯) = 5, but it does not tell us which value(s) of π‘₯ give 𝑓 (π‘₯) = 5. 84. For 𝑓 to be continuous at π‘₯ = 𝑐, we need limπ‘₯→𝑐 𝑓 (π‘₯) to exist and to be equal to 𝑓 (𝑐).


1.8 SOLUTIONS

95

85. We want a function which has a value at every point but where the graph has a break at π‘₯ = 15. One possibility is { 1 π‘₯ β‰₯ 15 𝑓 (π‘₯) = βˆ’1 π‘₯ < 15 86. One example is 𝑓 (π‘₯) = 1βˆ•π‘₯, which is not continuous at π‘₯ = 0. The Intermediate Value Theorem does not apply on an interval that contains a point where a function is not continuous. { 1 π‘₯≀2 87. Let 𝑓 (π‘₯) = . Then 𝑓 (π‘₯) is continuous at every point in [0, 3] except at π‘₯ = 2. Other answers are possible. π‘₯ π‘₯>2 { π‘₯ π‘₯≀3 88. Let 𝑓 (π‘₯) = . Then 𝑓 (π‘₯) is increasing for all π‘₯ but 𝑓 (π‘₯) is not continuous at π‘₯ = 3. Other answers are 2π‘₯ π‘₯ > 3 possible. { 1 π‘₯≀3 89. False. For example, let 𝑓 (π‘₯) = , then 𝑓 (π‘₯) is defined at π‘₯ = 3 but it is not continuous at π‘₯ = 3. (Other 2 π‘₯>3 examples are possible.) 90. False. A counterexample is graphed in Figure 1.111, in which 𝑓 (5) < 0. 𝑓 (π‘₯)

100

5

10

π‘₯

Figure 1.111 91. False. A counterexample is graphed in Figure 1.112. 𝑓 (π‘Ž)

𝑓 (π‘₯)

𝑓 (𝑏)

π‘Ž

𝑏

π‘₯

Figure 1.112

Solutions for Section 1.8 EXERCISES 1. (a) As π‘₯ approaches βˆ’1 from the right, 𝑓 (π‘₯) approaches 1. So lim+ 𝑓 (π‘₯) = 1. π‘₯β†’βˆ’1

(b) As π‘₯ approaches 0 from the left, 𝑓 (π‘₯) approaches 0. So limβˆ’ 𝑓 (π‘₯) = 0. π‘₯β†’0

(c) As π‘₯ approaches 0 from either side, 𝑓 (π‘₯) approaches 0, regardless of the fact that 𝑓 (0) = 2. So lim 𝑓 (π‘₯) = 0. π‘₯β†’0

(d) As π‘₯ approaches 1 from the left, 𝑓 (π‘₯) approaches 1. So limβˆ’ 𝑓 (π‘₯) = 1. π‘₯β†’1

(e) As π‘₯ approaches 1 from the left, 𝑓 (π‘₯) approaches 1. However, as π‘₯ approaches 1 from the right, 𝑓 (π‘₯) approaches 2. Since there is no single value that 𝑓 (π‘₯) approaches as π‘₯ approaches 1 from both sides, lim 𝑓 (π‘₯) does not exist. (f) As π‘₯ approaches 2 from the left, 𝑓 (π‘₯) approaches 1. So limβˆ’ 𝑓 (π‘₯) = 1. π‘₯β†’2

π‘₯β†’1


96

Chapter One /SOLUTIONS 2. (a) As π‘₯ approaches 1 from the left, the values of 𝑓 (π‘₯) get closer and closer to 1. So limβˆ’ 𝑓 (π‘₯) = 1. π‘₯β†’1

(b) As π‘₯ approaches 1 from the right, 𝑓 (π‘₯) goes to βˆ’βˆž. So limit does not exist since it does not approach a real number 𝐿, but we can use limit notation to say lim+ 𝑓 (π‘₯) = βˆ’βˆž. π‘₯β†’1

(c) As π‘₯ approaches 1 from the left, the values of 𝑓 (π‘₯) get closer and closer to 1. However, as π‘₯ approaches 1 from the right, 𝑓 (π‘₯) goes to βˆ’βˆž. Since there is no single value that 𝑓 (π‘₯) approaches as π‘₯ approaches 1 from both sides, lim 𝑓 (π‘₯) π‘₯β†’1

does not exist. (d) As π‘₯ approaches 2 from the left, the values of 𝑓 (π‘₯) get closer and closer to 1. So limβˆ’ 𝑓 (π‘₯) = 1. π‘₯β†’2

(e) As π‘₯ approaches 2 from the right, the values of 𝑓 (π‘₯) get closer and closer to 1. So lim+ 𝑓 (π‘₯) = 1. π‘₯β†’2

(f) As π‘₯ approaches 2 from either side, 𝑓 (π‘₯) approaches 1, regardless of the fact that 𝑓 (2) is undefined. So lim 𝑓 (π‘₯) = 1. π‘₯β†’2

3. (a) When π‘₯ = βˆ’2, we see that 𝑦 = 4. Therefore, 𝑓 (βˆ’2) = 4. (b) When π‘₯ = 0, we see that 𝑦 = 2. Therefore, 𝑓 (0) = 2. (c) As π‘₯ approaches βˆ’4 from the right, 𝑓 (π‘₯) approaches βˆ’4. Therefore, lim+ 𝑓 (π‘₯) = βˆ’4. π‘₯β†’βˆ’4

(d) As π‘₯ approaches βˆ’2 from the left, 𝑓 (π‘₯) approaches 2. Therefore, limβˆ’ 𝑓 (π‘₯) = 2. π‘₯β†’βˆ’2

(e) As π‘₯ approaches βˆ’2 from the right, 𝑓 (π‘₯) approaches 4. Therefore, lim+ 𝑓 (π‘₯) = 4. π‘₯β†’βˆ’2

(f) As π‘₯ approaches 0 from both sides, 𝑓 (π‘₯) approaches 0. Therefore, lim 𝑓 (π‘₯) = 0. π‘₯β†’0

(g) As π‘₯ approaches 2 from the left, 𝑓 (π‘₯) approaches 2. However, as π‘₯ approaches 2 from the right, 𝑓 (π‘₯) approaches 4. Therefore, lim 𝑓 (π‘₯) does not exist. π‘₯β†’2

(h) As π‘₯ approaches 4 from the left, 𝑓 (π‘₯) approaches 2. Therefore, limβˆ’ 𝑓 (π‘₯) = 2. π‘₯β†’4

4. (a) When π‘₯ = 0, there is no corresponding value of 𝑦 on the graph of 𝑓 . Therefore, 𝑓 (0) is undefined. (b) When π‘₯ = 4, we see that 𝑦 = βˆ’2. Therefore, 𝑓 (4) = βˆ’2. (c) As π‘₯ approaches βˆ’2 from the left, 𝑓 (π‘₯) approaches 2. Therefore, limβˆ’ 𝑓 (π‘₯) = 2. π‘₯β†’βˆ’2

(d) As π‘₯ approaches βˆ’2 from the right, 𝑓 (π‘₯) approaches βˆ’2. Therefore, lim+ 𝑓 (π‘₯) = βˆ’2. π‘₯β†’βˆ’2

(e) From parts (c) and (d), we see that limβˆ’ 𝑓 (π‘₯) is not equal to lim+ 𝑓 (π‘₯). Therefore, lim 𝑓 (π‘₯) does not exist. π‘₯β†’βˆ’2

π‘₯β†’βˆ’2

π‘₯β†’βˆ’2

(f) As π‘₯ approaches 0 from both sides, 𝑓 (π‘₯) approaches 2. Therefore, lim 𝑓 (π‘₯) = 2. π‘₯β†’0

(g) As π‘₯ approaches 2 from the left, 𝑓 (π‘₯) approaches βˆ’βˆž. Therefore, limβˆ’ 𝑓 (π‘₯) = βˆ’βˆž. π‘₯β†’2

(h) As π‘₯ approaches 2 from the right, 𝑓 (π‘₯) approaches ∞. Therefore, lim+ 𝑓 (π‘₯) = ∞. π‘₯β†’2

(i) From parts (g) and (h), we see that limβˆ’ 𝑓 (π‘₯) is not equal to lim+ 𝑓 (π‘₯). Therefore, lim 𝑓 (π‘₯) does not exist. π‘₯β†’2

π‘₯β†’2

π‘₯β†’2

(j) As π‘₯ approaches 4 from the left, 𝑓 (π‘₯) approaches 2. However, as π‘₯ approaches 4 from the right, 𝑓 (π‘₯) approaches βˆ’2. Therefore, lim 𝑓 (π‘₯) does not exist. π‘₯β†’4

5. (a) As π‘₯ gets larger and larger, the values of 𝑓 (π‘₯) oscillate, but the oscillations get smaller and smaller around 3. Therefore, we estimate that lim 𝑓 (π‘₯) = 3 π‘₯β†’βˆž

(b) As π‘₯ gets larger and larger in magnitude but negative, the values of 𝑓 (π‘₯) get larger and larger in magnitude but negative, so the 𝑓 (π‘₯) does not approach a real number, so the limit does not exist. Alternatively, we can say lim 𝑓 (π‘₯) = βˆ’βˆž. π‘₯β†’βˆ’βˆž

6. Using Theorem 1.2 we have, lim(𝑓 (π‘₯) βˆ’ 2β„Ž(π‘₯)) = lim 𝑓 (π‘₯) βˆ’ lim 2β„Ž(π‘₯)

Property 2

= lim 𝑓 (π‘₯) βˆ’ 2 lim β„Ž(π‘₯) π‘₯β†’2 π‘₯β†’2 1 = 7 βˆ’ 2 β‹… = 6. 2

Property 1

π‘₯β†’2

π‘₯β†’2

π‘₯β†’2

7. Using Theorem 1.2 we have, lim(𝑔(π‘₯))2 = lim(𝑔(π‘₯) β‹… 𝑔(π‘₯)) π‘₯β†’2

π‘₯β†’2

= (lim 𝑔(π‘₯)) β‹… (lim 𝑔(π‘₯)) Property 3 π‘₯β†’2

π‘₯β†’2

= (βˆ’4)(βˆ’4) = 16. 8. Using Theorem 1.2 we have, lim

𝑓 (π‘₯)

π‘₯β†’2 𝑔(π‘₯) β‹… β„Ž(π‘₯)

=

limπ‘₯β†’2 𝑓 (π‘₯) limπ‘₯β†’2 (𝑔(π‘₯) β‹… β„Ž(π‘₯))

Property 4


1.8 SOLUTIONS limπ‘₯β†’2 𝑓 (π‘₯) (limπ‘₯β†’2 𝑔(π‘₯))(limπ‘₯β†’2 β„Ž(π‘₯)) 7 7 =βˆ’ . = 1 2 (βˆ’4)( 2 ) =

9. We have

97

Property 3

lim(𝑓 (π‘₯) + 𝑔(π‘₯)) = lim 𝑓 (π‘₯) + lim 𝑔(π‘₯) = 27 + 3 = 30. π‘₯→𝑐

10. We have

π‘₯→𝑐

π‘₯→𝑐

lim(𝑓 (π‘₯) βˆ’ 𝑔(π‘₯)) = lim 𝑓 (π‘₯) βˆ’ lim 𝑔(π‘₯) = 27 βˆ’ 3 = 24. π‘₯→𝑐

11. We have

π‘₯→𝑐

π‘₯→𝑐

lim(𝑓 (π‘₯)𝑔(π‘₯)) = lim(𝑓 (π‘₯)) β‹… lim(𝑔(π‘₯)) = 27 β‹… 3 = 81. π‘₯→𝑐

π‘₯→𝑐

12. Since limπ‘₯→𝑐 𝑔(π‘₯) β‰  0, we have

( lim π‘₯→𝑐

13. We have

𝑓 (π‘₯) 𝑔(π‘₯)

π‘₯→𝑐

) =

limπ‘₯→𝑐 𝑓 (π‘₯) 27 = = 9. limπ‘₯→𝑐 𝑔(π‘₯) 3

( ) lim 10(𝑓 (π‘₯) βˆ’ 𝑔(π‘₯)) = 10 lim 𝑓 (π‘₯) βˆ’ lim 𝑔(π‘₯) = 10 (27 βˆ’ 3) = 240. π‘₯→𝑐

14. We have

π‘₯→𝑐

π‘₯→𝑐

( )( ) lim(𝑔(π‘₯))2 = lim(𝑔(π‘₯) β‹… 𝑔(π‘₯)) = lim 𝑔(π‘₯) lim 𝑔(π‘₯) = 32 = 9. π‘₯→𝑐

π‘₯→𝑐

π‘₯→𝑐

π‘₯→𝑐

15. From the graphs of 𝑓 and 𝑔, we estimate limβˆ’ 𝑓 (π‘₯) = 3, limβˆ’ 𝑔(π‘₯) = 5, π‘₯β†’1

lim+ 𝑓 (π‘₯) = 4, lim+ 𝑔(π‘₯) = 1.

π‘₯β†’1

π‘₯β†’1

π‘₯β†’1

(a) Using Theorem 1.2 we have limβˆ’ (𝑓 (π‘₯) + 𝑔(π‘₯)) = 3 + 5 = 8. π‘₯β†’1

(b) Using Theorem 1.2 we have lim+ (𝑓 (π‘₯) + 2𝑔(π‘₯)) = lim+ 𝑓 (π‘₯) + 2 lim+ 𝑔(π‘₯) = 4 + 2(1) = 6 π‘₯β†’1

π‘₯β†’1

π‘₯β†’1

(c) Using Theorem 1.2 we have limβˆ’ (𝑓 (π‘₯)𝑔(π‘₯)) = ( limβˆ’ 𝑓 (π‘₯))( limβˆ’ 𝑔(π‘₯)) = (3)(5) = 15 π‘₯β†’1 π‘₯β†’1 π‘₯β†’1 ( ) ( ) (d) Using Theorem 1.2 we have lim+ (𝑓 (π‘₯)βˆ•π‘”(π‘₯)) = lim+ 𝑓 (π‘₯) βˆ• lim+ 𝑔(π‘₯) = 4βˆ•1 = 4 π‘₯β†’1

π‘₯β†’1

π‘₯β†’1

16. We see that 𝑓 (π‘₯) goes to βˆ’βˆž on both ends, so one possible graph is shown in Figure 1.113. Other answers are possible.

π‘₯

Figure 1.113 17. We see that 𝑓 (π‘₯) goes to ∞ on the left and to βˆ’βˆž on the right. One possible graph is shown in Figure 1.114. Other answers are possible.

π‘₯

Figure 1.114


98

Chapter One /SOLUTIONS

18. We see that 𝑓 (π‘₯) goes to ∞ on the left and approaches a 𝑦-value of 1 on the right. One possible graph is shown in Figure 1.115. Other answers are possible. 𝑦

1

π‘₯

Figure 1.115

19. We see that 𝑓 (π‘₯) approaches a 𝑦-value of 3 on the left and goes to βˆ’βˆž on the right. One possible graph is shown in Figure 1.116. Other answers are possible. 𝑦 3 π‘₯

Figure 1.116

20. We see that 𝑓 (π‘₯) goes to ∞ on the right and that it also passes through the point (βˆ’1, 2). (Notice that this must be a point on the graph since the instructions require that 𝑓 (π‘₯) be defined and continuous.) One possible graph is shown in Figure 1.117. Other answers are possible.

2 π‘₯

βˆ’1

Figure 1.117

21. We see that 𝑓 (π‘₯) goes to ∞ on the left and that it also passes through the point (3, 5). (Notice that this must be a point on the graph since the instructions require that 𝑓 (π‘₯) be defined and continuous.) One possible graph is shown in Figure 1.118. Other answers are possible.

5 3

Figure 1.118

π‘₯


1.8 SOLUTIONS

99

22. We have lim π‘₯2 = ∞ because π‘₯2 increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large and π‘₯β†’βˆž positive. 23. We have lim π‘₯2 = ∞ because π‘₯2 increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large in π‘₯β†’βˆ’βˆž magnitude and negative. 24. We have lim π‘₯3 = βˆ’βˆž because π‘₯3 decreases and becomes arbitrarily large in magnitude and negative as π‘₯ becomes π‘₯β†’βˆ’βˆž arbitrarily large in magnitude and negative. 25. We have lim π‘₯3 = ∞ because π‘₯3 increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large and π‘₯β†’βˆž positive. 26. We have lim 𝑒π‘₯ = ∞ because 𝑒π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large and π‘₯β†’βˆž positive. 1 27. We have lim π‘’βˆ’π‘₯ = lim π‘₯ = 0 because 𝑒π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily π‘₯β†’βˆž π‘₯β†’βˆž 𝑒 large and positive, so 1βˆ•π‘’π‘₯ gets closer and closer to 0 as π‘₯ becomes arbitrarily large and positive. 1 28. We have lim 5βˆ’π‘₯ = lim π‘₯ = 0 because 5π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily π‘₯β†’βˆž π‘₯β†’βˆž 5 large and positive, so 1βˆ•5π‘₯ gets closer and closer to 0 as π‘₯ becomes arbitrarily large and positive. √ √ 29. We have lim π‘₯ = ∞ because π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large and π‘₯β†’βˆž positive. 30. We have lim ln π‘₯ = ∞ because ln π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily large and π‘₯β†’βˆž positive. 1 31. We have lim π‘₯βˆ’2 = lim 2 = 0 because π‘₯2 increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily π‘₯β†’βˆž π‘₯β†’βˆž π‘₯ large and positive, so 1βˆ•π‘₯2 gets closer and closer to 0 as π‘₯ becomes arbitrarily large and positive. 1 32. We have lim π‘₯βˆ’2 = lim 2 = 0 because π‘₯2 increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily π‘₯β†’βˆ’βˆž π‘₯β†’βˆ’βˆž π‘₯ large in magnitude and negative, so 1βˆ•π‘₯2 gets closer and closer to 0 as π‘₯ becomes arbitrarily large in magnitude and negative. 1 33. We have lim π‘₯βˆ’3 = lim 3 = 0 because π‘₯3 decreases and becomes arbitrarily large in magnitude and negative as π‘₯ π‘₯β†’βˆ’βˆž π‘₯β†’βˆ’βˆž π‘₯ becomes arbitrarily large in magnitude and negative, so 1βˆ•π‘₯3 gets closer and closer to 0 as π‘₯ becomes arbitrarily large in magnitude and negative. ( )π‘₯ 1 1 = lim π‘₯ = 0 because 2π‘₯ increases and becomes arbitrarily large and positive as π‘₯ becomes arbitrarily 34. We have lim π‘₯β†’βˆž 2 π‘₯β†’βˆž 2 large and positive, so 1βˆ•2π‘₯ gets closer and closer to 0 as π‘₯ becomes arbitrarily large and positive. 35. We see that lim 𝑓 (π‘₯) = βˆ’βˆž and lim 𝑓 (π‘₯) = βˆ’βˆž. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

36. As π‘₯ β†’ ±∞, we know that 𝑓 (π‘₯) behaves like its leading term βˆ’2π‘₯3 . Thus, we have lim 𝑓 (π‘₯) = ∞ and lim 𝑓 (π‘₯) = βˆ’βˆž. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

37. As π‘₯ β†’ ±∞, we know that 𝑓 (π‘₯) behaves like its leading term π‘₯5 . Thus, we have lim 𝑓 (π‘₯) = βˆ’βˆž and lim 𝑓 (π‘₯) = ∞. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

38. As π‘₯ β†’ ±∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since 𝑓 (π‘₯) β†’

3 3π‘₯3 = , 5 5π‘₯3

we have lim 𝑓 (π‘₯) = 3βˆ•5 and lim 𝑓 (π‘₯) = 3βˆ•5. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

39. As π‘₯ β†’ ±∞, we know that π‘₯βˆ’3 gets closer and closer to zero, so we have lim 𝑓 (π‘₯) = 0 and lim 𝑓 (π‘₯) = 0. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

40. We have lim 𝑓 (π‘₯) = 0 and lim 𝑓 (π‘₯) = ∞. π‘₯β†’βˆ’βˆž

π‘₯β†’βˆž

|π‘₯| |π‘₯| |π‘₯| = 1 and limβˆ’ = βˆ’1, we say that lim does not exist. In addition 𝑓 (π‘₯) is not defined at 0. Therefore, 41. Since lim+ π‘₯β†’0 π‘₯β†’0 π‘₯ π‘₯β†’0 π‘₯ π‘₯ 𝑓 (π‘₯) is not continuous on any interval containing 0. { ⎧ π‘₯βˆ’4 π‘₯>4 |π‘₯ βˆ’ 4| βŽͺ π‘₯ βˆ’ 4 1 π‘₯>4 =⎨ π‘₯βˆ’4 = 42. 𝑓 (π‘₯) = π‘₯βˆ’4 βˆ’1 π‘₯ < 4 π‘₯<4 βŽͺβˆ’ ⎩ π‘₯βˆ’4 Figure 1.119 confirms that lim+ 𝑓 (π‘₯) = 1, limβˆ’ 𝑓 (π‘₯) = βˆ’1 so lim 𝑓 (π‘₯) does not exist. π‘₯β†’4

π‘₯β†’4

π‘₯β†’4


100

Chapter One /SOLUTIONS 𝑓 (π‘₯)

1

0

2

4

6

π‘₯

8

βˆ’1

Figure 1.119 ⎧ π‘₯βˆ’2 , π‘₯>2 βŽͺ π‘₯ |π‘₯ βˆ’ 2| βŽͺ 43. 𝑓 (π‘₯) = =⎨ π‘₯ βŽͺ π‘₯βˆ’2 βŽͺβˆ’ π‘₯ , π‘₯ < 2 ⎩ Figure 1.120 confirms that lim+ 𝑓 (π‘₯) = limβˆ’ 𝑓 (π‘₯) = lim 𝑓 (π‘₯) = 0. π‘₯β†’2

π‘₯β†’2

π‘₯β†’2

1

𝑓 (π‘₯)

0

1

2

3

4

π‘₯

Figure 1.120 ⎧ π‘₯2 βˆ’ 2 0 < π‘₯ < 3 βŽͺ 44. 𝑓 (π‘₯) = ⎨ 2 π‘₯=3 βŽͺ 3<π‘₯ ⎩ 2π‘₯ + 1 Figure 1.121 confirms that limβˆ’ 𝑓 (π‘₯) = limβˆ’ (π‘₯2 βˆ’ 2) = 7 and that lim 𝑓 (π‘₯) = lim (2π‘₯ + 1) = 7, so lim 𝑓 (π‘₯) = 7. π‘₯β†’3

π‘₯β†’3

π‘₯β†’3+

Note, however, that 𝑓 (π‘₯) is not continuous at π‘₯ = 3 since 𝑓 (3) = 2. 𝑦 10 8 6 4 2 0 βˆ’2

𝑓 (π‘₯)

1

2

3

4

5

π‘₯

Figure 1.121 45. Yes. Since lim 𝑓 (π‘₯) = limβˆ’ (π‘₯2 + 1) = 2

π‘₯β†’1βˆ’

π‘₯β†’1

lim+ 𝑓 (π‘₯) = lim+ 2π‘₯ = 2,

π‘₯β†’1

π‘₯β†’1

we define 𝑓 (1) = 2. 46. No. Since lim 𝑓 (π‘₯) = limβˆ’ (4 βˆ’ π‘₯2 ) = 3

π‘₯β†’1βˆ’

π‘₯β†’1

lim+ 𝑓 (π‘₯) = lim+ (π‘₯ + 1) = 2.

π‘₯β†’1

π‘₯β†’1

π‘₯β†’3+

π‘₯β†’3


1.8 SOLUTIONS

101

47. Yes. Since lim 𝑓 (π‘₯) = limβˆ’ (π‘₯ βˆ’ 1) = 0

π‘₯β†’1βˆ’

π‘₯β†’1

lim+ 𝑓 (π‘₯) = lim+ (2 βˆ’ 2π‘₯) = 0,

π‘₯β†’1

π‘₯β†’1

we define 𝑓 (1) = 0. 48. No. Since 1 = Not defined (or +∞) 1βˆ’π‘₯ lim+ 𝑓 (π‘₯) = lim+ π‘₯ = 1.

lim 𝑓 (π‘₯) = limβˆ’

π‘₯β†’1βˆ’

π‘₯β†’1

π‘₯β†’1

π‘₯β†’1

PROBLEMS 49. The graph in Figure 1.122 suggests that as π‘₯ grows large, the value of (1 + 1βˆ•π‘₯)π‘₯ approaches a limit, which appears to be slightly greater than 2.7. If we zoom out further, we see it appears to be about 2.72, which is close to the value of 𝑒 β‰ˆ 2.71828. Thus we guess that lim (1 + 1βˆ•π‘₯)π‘₯ = 𝑒 π‘₯β†’βˆž

𝑦 5

𝑦=𝑒

𝑓 (π‘₯) = (1 + 1βˆ•π‘₯)π‘₯

βˆ’10

10

100

π‘₯

Figure 1.122 50. We use values of π‘₯ approaching ∞ and make a table. We see that as π‘₯ grows very large, the value of (1 + 1βˆ•π‘₯)π‘₯ appears to approach a value close to 2.7183. We recognize this value as 𝑒 rounded to four decimal places, so we estimate lim (1 + π‘₯β†’βˆž

1βˆ•π‘₯)π‘₯ = 𝑒. π‘₯

1

10

100

1000

10000

100000

1000000

(1 + 1βˆ•π‘₯)π‘₯

2.0000

2.5937

2.7048

2.7169

2.7181

2.7183

2.7183

51. (a)

10

5

βˆ’10

βˆ’5

5

10

π‘₯

Figure 1.123 (b) The graph of 𝑓 (π‘₯) suggests that it is not continuous at π‘₯ = 0. However, the function 𝑓 (π‘₯) is the composition of a rational function 1βˆ•(π‘₯2 + 0.0001), which is continuous everywhere since its denominator is never zero, with the exponential function 𝑒π‘₯ , which is continuous everywhere. Therefore 𝑓 (π‘₯) is continuous everywhere, so must be continuous at π‘₯ = 0.


Chapter One /SOLUTIONS

102

52. When π‘₯ = 0.1, we find π‘₯𝑒1βˆ•π‘₯ β‰ˆ 2203. When π‘₯ = 0.01, we find π‘₯𝑒1βˆ•π‘₯ β‰ˆ 3 Γ— 1041 . When π‘₯ = 0.001, the value of π‘₯𝑒1βˆ•π‘₯ is too big for a calculator to compute. This suggests that lim+ π‘₯𝑒1βˆ•π‘₯ does not exist (and in fact it does not). π‘₯β†’0

53. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π‘₯ 𝑓 (π‘₯) β†’ = βˆ’1, βˆ’π‘₯ we have lim 𝑓 (π‘₯) = βˆ’1. π‘₯β†’βˆž Alternatively, we could divide numerator and denominator by π‘₯ and apply the properties of limits: 𝑓 (π‘₯) = so

1 + 3βˆ•π‘₯ π‘₯+3 = , 2βˆ’π‘₯ 2βˆ•π‘₯ βˆ’ 1

lim (1 + 3βˆ•π‘₯) lim 1 + lim (3βˆ•π‘₯) 1 + 3βˆ•π‘₯ π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 1 = = = βˆ’1 = π‘₯β†’βˆž 2βˆ•π‘₯ βˆ’ 1 lim (2βˆ•π‘₯ βˆ’ 1) lim (2βˆ•π‘₯) βˆ’ lim 1 βˆ’1

lim 𝑓 (π‘₯) = lim

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

since 1βˆ•π‘₯ β†’ 0 as π‘₯ β†’ ∞. 54. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since 𝑓 (π‘₯) β†’

3 3π‘₯ = , πœ‹π‘₯ πœ‹

we have lim 𝑓 (π‘₯) = 3βˆ•πœ‹. π‘₯β†’βˆž Alternatively, we could divide numerator and denominator by π‘₯ and apply the properties of limits: πœ‹βˆ•π‘₯ + 3 πœ‹ + 3π‘₯ = , πœ‹π‘₯ βˆ’ 3 πœ‹ βˆ’ 3βˆ•π‘₯

𝑓 (π‘₯) = so

lim (πœ‹βˆ•π‘₯ + 3) lim (πœ‹βˆ•π‘₯) + lim 3 πœ‹βˆ•π‘₯ + 3 π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 3 = = = π‘₯β†’βˆž πœ‹ βˆ’ 3βˆ•π‘₯ lim (πœ‹ βˆ’ 3βˆ•π‘₯) lim πœ‹ βˆ’ lim (3βˆ•π‘₯) πœ‹

lim 𝑓 (π‘₯) = lim

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

since π‘Žβˆ•π‘₯ β†’ 0 as π‘₯ β†’ ∞ for any nonzero number π‘Ž.. 55. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since 𝑓 (π‘₯) β†’

1 π‘₯ = , 2π‘₯ 2π‘₯2

we have lim 𝑓 (π‘₯) = 0 because 1βˆ•(2π‘₯) β†’ 0 as π‘₯ β†’ ∞. π‘₯β†’βˆž

Alternatively, we could divide numerator and denominator by π‘₯2 and apply the properties of limits: 𝑓 (π‘₯) =

1βˆ•π‘₯ βˆ’ 5βˆ•π‘₯2 π‘₯βˆ’5 , = 5 + 2π‘₯2 5βˆ•π‘₯2 + 2

) ( lim (1βˆ•π‘₯) βˆ’ lim (5βˆ•π‘₯2 ) lim (1βˆ•π‘₯) βˆ’ (5βˆ•π‘₯2 ) 1βˆ•π‘₯ βˆ’ 5βˆ•π‘₯2 π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 0 = =0 lim 𝑓 (π‘₯) = lim = ) = ( π‘₯β†’βˆž π‘₯β†’βˆž 5βˆ•π‘₯2 + 2 2 lim (5βˆ•π‘₯2 ) + lim 2 lim (5βˆ•π‘₯2 ) + 2

so

π‘₯β†’βˆž

since lim π‘Žβˆ•π‘₯𝑛 = 0 for any nonzero number π‘Ž and positive 𝑛.

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

56. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since 𝑓 (π‘₯) β†’

1 π‘₯2 = , 3 3π‘₯2

we have lim 𝑓 (π‘₯) = 1βˆ•3. π‘₯β†’βˆž

Alternatively, we could divide numerator and denominator by π‘₯2 and apply the properties of limits: 𝑓 (π‘₯) =

1 + 2βˆ•π‘₯ βˆ’ 1βˆ•π‘₯2 π‘₯2 + 2π‘₯ βˆ’ 1 , = 2 3 + 3π‘₯ 3βˆ•π‘₯2 + 3

( ) lim 1 + lim (2βˆ•π‘₯) βˆ’ lim (1βˆ•π‘₯2 ) lim 1 + 2βˆ•π‘₯ βˆ’ 1βˆ•π‘₯2 1 + 2βˆ•π‘₯ βˆ’ 1βˆ•π‘₯2 π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 1 lim 𝑓 (π‘₯) = lim = = = ) ( π‘₯β†’βˆž π‘₯β†’βˆž 3 3βˆ•π‘₯2 + 3 lim (3βˆ•π‘₯2 ) + lim 3 lim 3βˆ•π‘₯2 + 3

so

π‘₯β†’βˆž

since lim π‘Žβˆ•π‘₯𝑛 = 0 for any nonzero number π‘Ž and positive 𝑛. π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž


1.8 SOLUTIONS

103

57. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π‘₯2 = π‘₯, π‘₯

𝑓 (π‘₯) β†’

we have lim 𝑓 (π‘₯) = ∞. π‘₯β†’βˆž Alternatively, we could divide numerator and denominator by π‘₯ and apply the properties of limits: π‘₯ + 4βˆ•π‘₯ π‘₯2 + 4 = , π‘₯+3 1 + 3βˆ•π‘₯

𝑓 (π‘₯) = so

lim (π‘₯ + 4βˆ•π‘₯) lim π‘₯ + lim (4βˆ•π‘₯) π‘₯ + 4βˆ•π‘₯ π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž = = lim π‘₯ = ∞ = π‘₯β†’βˆž 1 + 3βˆ•π‘₯ lim (1 + 3βˆ•π‘₯) lim 1 + lim (3βˆ•π‘₯) π‘₯β†’βˆž

lim 𝑓 (π‘₯) = lim

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

since lim π‘Žβˆ•π‘₯ = 0 for any nonzero number π‘Ž. π‘₯β†’βˆž

58. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since 𝑓 (π‘₯) β†’

2π‘₯3 2 = , 3 3π‘₯3

we have lim 𝑓 (π‘₯) = 2βˆ•3. π‘₯β†’βˆž

Alternatively, we could divide numerator and denominator by π‘₯3 and apply the properties of limits: 𝑓 (π‘₯) = so

2 βˆ’ 16βˆ•π‘₯ 2π‘₯3 βˆ’ 16π‘₯2 = , 2 3 4βˆ•π‘₯ + 3 4π‘₯ + 3π‘₯

lim (2 βˆ’ 16βˆ•π‘₯) lim 2 βˆ’ lim (16βˆ•π‘₯) 2 βˆ’ 16βˆ•π‘₯ π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 2 = = = π‘₯β†’βˆž 4βˆ•π‘₯ + 3 lim (4βˆ•π‘₯ + 3) lim (4βˆ•π‘₯) + lim 3 3

lim 𝑓 (π‘₯) = lim

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

since lim π‘Žβˆ•π‘₯ = 0 for any nonzero number π‘Ž. π‘₯β†’βˆž

59. As π‘₯ β†’ ∞, we know that 𝑓 (π‘₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π‘₯4 1 = , 2π‘₯ 2π‘₯5

𝑓 (π‘₯) β†’ we have lim 𝑓 (π‘₯) = 0 because 1βˆ•(2π‘₯) β†’ 0 as π‘₯ β†’ ∞. π‘₯β†’βˆž

Alternatively, we could divide numerator and denominator by π‘₯5 and apply the properties of limits: 𝑓 (π‘₯) =

1βˆ•π‘₯ + 3βˆ•π‘₯4 π‘₯4 + 3π‘₯ = , 4 5 1βˆ•π‘₯ + 2 π‘₯ + 2π‘₯

( ) lim 1βˆ•π‘₯ + 3βˆ•π‘₯4

so lim 𝑓 (π‘₯) =

π‘₯β†’βˆž

π‘₯β†’βˆž

lim (1βˆ•π‘₯ + 2)

lim (1βˆ•π‘₯) + lim (3βˆ•π‘₯4 )

=

π‘₯β†’βˆž

π‘₯β†’βˆž

=

lim (1βˆ•π‘₯) + lim 2

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

0 =0 2

since lim π‘Žβˆ•π‘₯𝑛 = 0 for any nonzero number π‘Ž and positive 𝑛. π‘₯β†’βˆž

60. For large values of π‘₯, 3𝑒π‘₯ + 2 behaves like 3𝑒π‘₯ and 2𝑒π‘₯ + 3 behaves like 2𝑒π‘₯ , so for large values of π‘₯, 𝑓 (π‘₯) β†’

3 3𝑒π‘₯ = . 2𝑒π‘₯ 2

Thus we have we have lim 𝑓 (π‘₯) = 3βˆ•2. π‘₯β†’βˆž Alternatively, we could divide numerator and denominator by 𝑒π‘₯ and apply the properties of limits: 𝑓 (π‘₯) = so

3 + 2π‘’βˆ’π‘₯ 3𝑒π‘₯ + 2 , = 2𝑒π‘₯ + 3 2 + 3π‘’βˆ’π‘₯

lim (3 + 2π‘’βˆ’π‘₯ )

lim 𝑓 (π‘₯) =

π‘₯β†’βˆž

π‘₯β†’βˆž π‘₯β†’βˆž

since lim π‘Žπ‘’βˆ’π‘₯ = 0 for any nonzero number π‘Ž. π‘₯β†’βˆž

lim (2 + 3π‘’βˆ’π‘₯ )

lim 3 + lim 2π‘’βˆ’π‘₯

=

π‘₯β†’βˆž

π‘₯β†’βˆž

lim 2 + lim 3π‘’βˆ’π‘₯

π‘₯β†’βˆž

π‘₯β†’βˆž

=

3 2


104

Chapter One /SOLUTIONS

61. Since lim 2βˆ’π‘₯ = lim 3βˆ’π‘₯ = 0, we have π‘₯β†’βˆž

π‘₯β†’βˆž

lim (2βˆ’π‘₯ + 5) lim 2βˆ’π‘₯ + lim 5 π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž 5 2βˆ’π‘₯ + 5 lim 𝑓 (π‘₯) = lim βˆ’π‘₯ = = = . π‘₯β†’βˆž π‘₯β†’βˆž 3 +7 lim (3βˆ’π‘₯ + 7) lim 3βˆ’π‘₯ + lim 7 7 π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

62. Since lim π‘Žπ‘’βˆ’π‘₯ = 0 for any nonzero π‘Ž, we have π‘₯β†’βˆž

lim (2π‘’βˆ’π‘₯ + 3)

lim 𝑓 (π‘₯) =

π‘₯β†’βˆž

π‘₯β†’βˆž

lim (3π‘’βˆ’π‘₯ + 2)

lim 2π‘’βˆ’π‘₯ + lim 3

=

π‘₯β†’βˆž

π‘₯β†’βˆž

π‘₯β†’βˆž

lim 3π‘’βˆ’π‘₯ + lim 2

π‘₯β†’βˆž

π‘₯β†’βˆž

=

3 . 2

63. (a) Figure 1.124 shows a possible graph of 𝑓 (π‘₯), yours may be different. 9

2 3

π‘₯

5

Figure 1.124 (b) In order for 𝑓 to approach the horizontal asymptote at 9 from above it is necessary that 𝑓 eventually become concave up. It is therefore not possible for 𝑓 to be concave down for all π‘₯ > 6. 64. One possible graph is shown in Figure 1.125. Other answers are possible. 𝑦 4

βˆ’4

π‘₯

4 βˆ’2

Figure 1.125 65. One possible graph is shown in Figure 1.126. Other answers are possible. 𝑦 4

βˆ’5

5 βˆ’3

Figure 1.126

π‘₯


1.8 SOLUTIONS

105

66. (a) We know that lim 𝑓 (π‘₯) does not exist for π‘Ž = 3. Since the graph of 𝑓 (π‘₯) has a vertical asymptote at π‘₯ = 3, this π‘₯β†’π‘Ž

means that 𝑓 (π‘₯) approaches ∞ or βˆ’βˆž as π‘₯ approaches 3 from the right or from the left. This means that 𝑓 (π‘₯) cannot approach a finite real number as π‘₯ approaches 3 from both sides. (b) If lim 𝑓 (π‘₯) exists, then the graph of 𝑓 (π‘₯) must approach a horizontal asymptote as π‘₯ approaches ∞. Since the only π‘₯β†’βˆž

horizontal asymptote is 𝑦 = βˆ’4, the value of 𝑓 (π‘₯) must approach βˆ’4 as π‘₯ gets large. So lim 𝑓 (π‘₯) = βˆ’4. π‘₯β†’βˆž

67. (a)

(i) As 𝑑 approaches 1 from the left, 𝑄 approaches 50. Therefore, limβˆ’ 𝑓 (𝑑) = 50. This means that the amount of the 𝑑→1

drug in the patient’s body is about 50 mg right before the second dose is taken. (ii) As 𝑑 approaches 1 from the right, 𝑄 approaches 150. Therefore, lim+ 𝑓 (𝑑) = 150. This means that the amount of 𝑑→1

drug in the patient’s body is about 150 mg right after the second dose is taken. (b) The function 𝑓 is discontinuous at 𝑑 = 1, 2, 3, and 4 days. These points of discontinuity occur at the times when the drug is taken because the amount of the drug in the body suddenly increases at these times. 68. For all π‘₯ sufficiently close to π‘₯ = 1 but with π‘₯ > 1, we have 𝑝(π‘₯) = 14, so lim+ 𝑝(π‘₯) = 14. For all π‘₯ sufficiently close to π‘₯β†’1

π‘₯ = 1 but with π‘₯ < 1 we have 𝑝(π‘₯) = 7, so limβˆ’ 𝑝(π‘₯) = 7. Therefore, the one sided limits of 𝑝(π‘₯) at π‘₯ = 1 are different and π‘₯β†’1

so lim 𝑝(π‘₯) does not exist. π‘₯β†’1

69. We calculate this limit in stages, using the limit properties in Theorem 1.2 to justify each step: ) ( lim π‘₯2 + 5π‘₯ π‘₯β†’3 π‘₯2 + 5π‘₯ (Property 4, since limπ‘₯β†’3 (π‘₯ + 9) β‰  0) lim = π‘₯β†’3 π‘₯ + 9 lim (π‘₯ + 9) π‘₯β†’3 ( ) lim π‘₯2 + lim (5π‘₯) π‘₯β†’3 π‘₯β†’3 = (Property 2) lim π‘₯ + lim 9 π‘₯β†’3 π‘₯β†’3 ( )2 ( ) lim π‘₯ + 5 lim π‘₯ π‘₯β†’3 π‘₯β†’3 = (Properties 1 and 3) lim π‘₯ + lim 9 π‘₯β†’3

π‘₯β†’3

32 + 5 β‹… 3 = = 2. 3+9

(Properties 5 and 6)

70. There are many possible correct answers. (a) If 𝑓 (π‘₯) = π‘₯2 and 𝑔(π‘₯) = π‘₯ then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = π‘₯ so lim

𝑓 (π‘₯)

π‘₯β†’βˆž 𝑔(π‘₯)

(b) If 𝑓 (π‘₯) = 3π‘₯ and 𝑔(π‘₯) = π‘₯ then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 3 so lim

𝑓 (π‘₯)

π‘₯β†’βˆž 𝑔(π‘₯)

(c) If 𝑓 (π‘₯) = π‘₯ and 𝑔(π‘₯) = π‘₯2 then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 1βˆ•π‘₯ so lim

= ∞. = 3.

𝑓 (π‘₯)

π‘₯β†’βˆž 𝑔(π‘₯)

= 0.

71. (a) We have π‘₯+5 10 10 1 = βˆ’ βˆ’ π‘₯ βˆ’ 5 π‘₯2 βˆ’ 5 (π‘₯ + 5)(π‘₯ βˆ’ 5) (π‘₯ + 5)(π‘₯ βˆ’ 5) π‘₯ + 5 βˆ’ 10 = (π‘₯ + 5)(π‘₯ βˆ’ 5) π‘₯βˆ’5 . = (π‘₯ + 5)(π‘₯ βˆ’ 5) (b) We have lim π‘₯β†’5

(

10 1 βˆ’ π‘₯ βˆ’ 5 π‘₯2 βˆ’ 25

)

π‘₯βˆ’5

= lim

π‘₯β†’5 (π‘₯ + 5)(π‘₯ βˆ’ 5)

= lim

1

π‘₯β†’5 π‘₯ + 5

=

1 1 = 5+5 10

Canceling π‘₯ βˆ’ 5 since π‘₯ β‰  5 in the limit Substituting π‘₯ = 5 since 1βˆ•(π‘₯ + 5) is continuous at π‘₯ = 5.


106

Chapter One /SOLUTIONS (c) Property 2 of Theorem 1.2 states lim(𝑓 (π‘₯) + 𝑔(π‘₯)) = lim 𝑓 (π‘₯) + lim 𝑔(π‘₯) π‘₯→𝑐

π‘₯→𝑐

π‘₯→𝑐

provided the limits on the right hand side exist. In this case, neither lim

1

π‘₯β†’5 π‘₯ βˆ’ 5

invoke the property.

10 exist, so we cannot nor lim βˆ’ 2 π‘₯β†’5 π‘₯ βˆ’ 25

72. The only change is that, instead of considering all π‘₯ near 𝑐, we only consider π‘₯ near to and greater than 𝑐. Thus we define limπ‘₯→𝑐 + 𝑓 (π‘₯), to be a number 𝐿 (if one exists) such that 𝑓 (π‘₯) is as close to 𝐿 as we want whenever π‘₯ is sufficiently close to 𝑐 and π‘₯ > 𝑐. 73. The only change is that, instead of considering all π‘₯ near 𝑐, we only consider π‘₯ near to and less than 𝑐. Thus we define limπ‘₯→𝑐 βˆ’ 𝑓 (π‘₯), to be a number 𝐿 (if one exists) such that 𝑓 (π‘₯) is as close to 𝐿 as we want whenever π‘₯ is sufficiently close to 𝑐 and π‘₯ < 𝑐. 74. If 𝑐 is in the interval, we know lim 𝑓 (π‘₯) = 𝑓 (𝑐) and limπ‘₯→𝑐 𝑔(π‘₯) = 𝑔(𝑐). Then, π‘₯→𝑐

lim (𝑓 (π‘₯) + 𝑔(π‘₯)) = lim 𝑓 (π‘₯) + lim 𝑔(π‘₯) Property 2 π‘₯→𝑐

π‘₯→𝑐

π‘₯→𝑐

= 𝑓 (𝑐) + 𝑔(𝑐),

so 𝑓 + 𝑔 is continuous at π‘₯ = 𝑐.

Also, lim (𝑓 (π‘₯)𝑔(π‘₯)) = lim 𝑓 (π‘₯) lim 𝑔(π‘₯) Property 3 π‘₯→𝑐

π‘₯→𝑐

π‘₯→𝑐

= 𝑓 (𝑐)𝑔(𝑐) so 𝑓 𝑔 is continuous at π‘₯ = 𝑐. Finally,

lim

𝑓 (π‘₯)

π‘₯→𝑐 𝑔(π‘₯)

limπ‘₯→𝑐 𝑓 (π‘₯) Property 4 limπ‘₯→𝑐 𝑔(π‘₯) 𝑓 (𝑐) 𝑓 = , so is continuous at π‘₯ = 𝑐. 𝑔(𝑐) 𝑔 =

Strengthen Your Understanding 75. Though 𝑃 (π‘₯) and 𝑄(π‘₯) are both continuous for all π‘₯, it is possible for 𝑄(π‘₯) to be equal to zero for some π‘₯. For any such value of π‘₯, where 𝑄(π‘₯) = 0, we see that 𝑃 (π‘₯)βˆ•π‘„(π‘₯) is undefined, and thus not continuous. For example, 𝑃 (π‘₯) π‘₯ = 𝑄(π‘₯) π‘₯βˆ’1 is not defined or continuous at π‘₯ = 1. 76. The left- and right-hand limits are not the same: lim

π‘₯βˆ’1

= βˆ’1,

lim

π‘₯βˆ’1

= 1.

π‘₯β†’1βˆ’ |π‘₯ βˆ’ 1|

but

π‘₯β†’1+ |π‘₯ βˆ’ 1|

Since the left- and right-hand limits are not the same, the limit does not exist and thus is not equal to 1. 77. One possibility is 𝑓 (π‘₯) = We have limπ‘₯β†’1 𝑓 (π‘₯) = 4 but 𝑓 (1) is undefined.

(π‘₯ + 3)(π‘₯ βˆ’ 1) . π‘₯βˆ’1

78. One example is 𝑓 (π‘₯) =

2|π‘₯| . π‘₯


1.8 SOLUTIONS

107

79. True, by Property 3 of limits in Theorem 1.2, since lim π‘₯ = 3. π‘₯β†’3

80. False. If lim 𝑔(π‘₯) does not exist, then lim 𝑓 (π‘₯)𝑔(π‘₯) may not even exist. For example, let 𝑓 (π‘₯) = 2π‘₯ + 1 and define 𝑔 by: π‘₯β†’3

π‘₯β†’3

{

1βˆ•(π‘₯ βˆ’ 3) if π‘₯ β‰  3 4 if π‘₯ = 3 Then lim 𝑓 (π‘₯) = 7 and 𝑔(3) = 4, but lim 𝑓 (π‘₯)𝑔(π‘₯) β‰  28, since lim(2π‘₯ + 1)βˆ•(π‘₯ βˆ’ 3) does not exist. 𝑔(π‘₯) =

π‘₯β†’3

π‘₯β†’3

π‘₯β†’3

81. True, by Property 2 of limits in Theorem 1.2. 82. True, by Properties 2 and 3 of limits in Theorem 1.2. lim 𝑔(π‘₯) = lim(𝑓 (π‘₯) + 𝑔(π‘₯) + (βˆ’1)𝑓 (π‘₯)) = lim (𝑓 (π‘₯) + 𝑔(π‘₯)) + (βˆ’1) lim 𝑓 (π‘₯) = 12 + (βˆ’1)7 = 5. π‘₯β†’3

π‘₯β†’3

π‘₯β†’3

π‘₯β†’3

83. True. Suppose instead that lim 𝑔(π‘₯) does not exist but lim(𝑓 (π‘₯)𝑔(π‘₯)) did exist. Since lim 𝑓 (π‘₯) exists and is not zero, then π‘₯β†’3

π‘₯β†’3

π‘₯β†’3

lim((𝑓 (π‘₯)𝑔(π‘₯))βˆ•π‘“ (π‘₯)) exists, by Property 4 of limits in Theorem 1.2. Furthermore, 𝑓 (π‘₯) β‰  0 for all π‘₯ in some interval π‘₯β†’3

about 3, so (𝑓 (π‘₯)𝑔(π‘₯))βˆ•π‘“ (π‘₯) = 𝑔(π‘₯) for all π‘₯ in that interval. Thus lim 𝑔(π‘₯) exists. This contradicts our assumption that π‘₯β†’3

lim 𝑔(π‘₯) does not exist. π‘₯β†’3

84. False, since the one-sided limits as π‘₯ β†’ 7 from both sides are unequal. 85. True, since the one-sided limits as π‘₯ β†’ 7 from both sides are equal to 4. 86. True, since the one-sided limits as π‘₯ β†’ 7 from both sides exist, th ratio of their limits is equal to βˆ’1. 87. False, since we don’t know if 𝑓 (π‘₯) or (𝑓 (π‘₯))2 is defined at π‘₯ = 7. 88. False, since limπ‘₯β†’7 𝑓 (π‘₯) does not exist. 89. True, since limπ‘₯β†’7 (𝑓 (π‘₯))2 = 4 and (𝑓 (7)2 ) = 4. 90. True, since as π‘₯ β†’ ∞, 1βˆ•π‘₯ β†’ 0 and as the sine function is continuous, sin(1βˆ•π‘₯) β†’ 0, so the product of the two has a limit of 0. 91. False, since as π‘₯ β†’ 0+ the function 1βˆ•π‘₯ β†’ ∞. Also, as π‘₯ β†’ ∞ the function sin(1βˆ•π‘₯) oscillates faster and faster between +1 and βˆ’1. Therefore the product of the two does not tend to either ∞ or βˆ’βˆž as π‘₯ β†’ 0 on either side, but instead oscillates between large positive and large negative values.

Additional Problems (online only) 2

92. The function 𝑓 (π‘₯) is the product of the rational function 1βˆ•(π‘₯2 βˆ’ 1) with 𝑒sin(3π‘₯ +2π‘₯βˆ’1) . The rational function is continuous so long as the denominator is not 0, that is, when π‘₯ β‰  Β±1. The other function is a composition of a polynomial, a sine, and an exponential, so is continuous over any interval. Therefore the product of these two functions is continuous over any interval that does not contain π‘₯ = Β±1. 93. We have

1 π‘₯ = , sin π‘₯ (sin π‘₯)βˆ•π‘₯

so, lim

π‘₯

π‘₯β†’0 sin π‘₯

=

limπ‘₯β†’0 1 1 = = 1. limπ‘₯β†’0 (sin π‘₯)βˆ•π‘₯ 1

94. We have sin π‘₯ = π‘₯ Therefore,

sin π‘₯ . π‘₯

) ( )( sin π‘₯ = 0 β‹… 1 = 0. lim sin π‘₯ = lim π‘₯ lim π‘₯β†’0 π‘₯β†’0 π‘₯β†’0 π‘₯

95. We have (sin 3π‘₯)βˆ•π‘₯ = 3(sin 3π‘₯)βˆ•(3π‘₯). If we let 𝑒 = 3π‘₯, then 𝑒 β†’ 0 as π‘₯ β†’ 0, so lim π‘₯β†’0

Thus lim π‘₯β†’0

sin 3π‘₯ sin 𝑒 = lim = 1. 𝑒→0 3π‘₯ 𝑒

sin 3π‘₯ sin 3π‘₯ = 3 lim = 3. π‘₯β†’0 3π‘₯ π‘₯


108

Chapter One /SOLUTIONS

96. We have

βˆ’ sin2 π‘₯ cos2 π‘₯ βˆ’ 1 = . π‘₯2 π‘₯2

Therefore

)( ) ( cos2 π‘₯ βˆ’ 1 sin π‘₯ sin π‘₯ lim = βˆ’1 = βˆ’ lim 2 π‘₯β†’0 π‘₯β†’0 π‘₯ π‘₯ π‘₯ 97. (a) This statement follows: if we interchange the roles of 𝑓 and 𝑔 in the original statement, we get this statement. (b) This statement is true, but it does not follow directly from the original statement, which says nothing about the case 𝑔(π‘Ž) = 0. (c) This follows, since if 𝑔(π‘Ž) β‰  0 the original statement would imply 𝑓 βˆ•π‘” is continuous at π‘₯ = π‘Ž, but we are told it is not. (d) This does not follow. Given that 𝑓 is continuous at π‘₯ = π‘Ž and 𝑔(π‘Ž) β‰  0, then the original statement says 𝑔 continuous implies 𝑓 βˆ•π‘” continuous, not the other way around. In fact, statement (d) is not true: if 𝑓 (π‘₯) = 0 for all π‘₯, then 𝑔 could be any discontinuous, non-zero function, and 𝑓 βˆ•π‘” would be zero, and therefore continuous. Thus the conditions of the statement would be satisfied, but not the conclusion. lim π‘₯β†’0

Solutions for Section 1.9 EXERCISES 1. Canceling, we have lim

3π‘₯2 = lim 3 = 3. π‘₯β†’0 π‘₯2

lim

3π‘₯2 = lim 3π‘₯ = 0. π‘₯β†’0 π‘₯

lim

3π‘₯2 3 = lim 2 = ∞. π‘₯β†’0 π‘₯ π‘₯4

π‘₯β†’0

2. Canceling, we have π‘₯β†’0

3. The limit does not exist since canceling, we have π‘₯β†’0

4. Factoring the numerator and simplifying, we get π‘₯(π‘₯ βˆ’ 3) π‘₯2 βˆ’ 3π‘₯ = =π‘₯ π‘₯βˆ’3 π‘₯βˆ’3 provided π‘₯ β‰  3. Thus lim π‘₯β†’3

π‘₯2 βˆ’ 3π‘₯ = lim π‘₯ = 3. π‘₯β†’3 π‘₯βˆ’3

5. Factoring the numerator and the denominator, we obtain 𝑑2 (𝑑2 + 1) 𝑑2 + 1 𝑑4 + 𝑑2 = = 2𝑑 βˆ’ 9 2𝑑3 βˆ’ 9𝑑2 𝑑2 (2𝑑 βˆ’ 9) provided 𝑑 β‰  0. Thus lim

𝑑4 + 𝑑2

𝑑→0 2𝑑3 βˆ’ 9𝑑2

6. Factoring the numerator, we obtain

provided π‘₯ β‰  0. Thus

= lim

𝑑2 + 1

𝑑→0 2𝑑 βˆ’ 9

1 =βˆ’ . 9

π‘₯(π‘₯2 βˆ’ 3) π‘₯2 βˆ’ 3 π‘₯3 βˆ’ 3π‘₯ = √ = √ √ 2π‘₯ + 3 π‘₯ 2π‘₯ + 3 π‘₯ 2π‘₯ + 3 √ 3 π‘₯3 βˆ’ 3π‘₯ π‘₯2 βˆ’ 3 lim √ = lim √ = βˆ’ √ = βˆ’ 3. π‘₯β†’0 π‘₯β†’0 π‘₯ 2π‘₯ + 3 2π‘₯ + 3 3


1.9 SOLUTIONS 7. Factoring the denominator and simplifying, we get π‘₯+4 π‘₯+4 1 = = (π‘₯ + 4)(2π‘₯ βˆ’ 3) 2π‘₯ βˆ’ 3 2π‘₯2 + 5π‘₯ βˆ’ 12 provided π‘₯ β‰  βˆ’4. Thus

π‘₯+4

lim

π‘₯β†’βˆ’4 2π‘₯2 + 5π‘₯ βˆ’ 12

= lim

1

π‘₯β†’βˆ’4 2π‘₯ βˆ’ 3

=βˆ’

1 . 11

8. Factoring the numerator and simplifying, we get (𝑦 βˆ’ 1)(𝑦 βˆ’ 4) 𝑦2 βˆ’ 5𝑦 + 4 = =π‘¦βˆ’4 π‘¦βˆ’1 π‘¦βˆ’1 provided 𝑦 β‰  1. Thus

𝑦2 βˆ’ 5𝑦 + 4 = lim(𝑦 βˆ’ 4) = βˆ’3. 𝑦→1 𝑦→1 π‘¦βˆ’1

lim

9. Factoring the numerator and denominator and simplifying, we get (π‘₯ βˆ’ 1)(π‘₯ + 3) π‘₯+3 π‘₯2 + 2π‘₯ βˆ’ 3 = = (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 2) π‘₯βˆ’2 π‘₯2 βˆ’ 3π‘₯ + 2 provided π‘₯ β‰  1. Thus

π‘₯2 + 2π‘₯ βˆ’ 3 π‘₯+3 = lim = βˆ’4. π‘₯β†’1 π‘₯2 βˆ’ 3π‘₯ + 2 π‘₯β†’1 π‘₯ βˆ’ 2

lim

10. Factoring the numerator and denominator and simplifying, we get (𝑑 + 2)(2𝑑 βˆ’ 1) 2𝑑 βˆ’ 1 2𝑑2 + 3𝑑 βˆ’ 2 = = (𝑑 + 2)(𝑑 + 3) 𝑑+3 𝑑2 + 5𝑑 + 6 provided 𝑑 β‰  βˆ’2. Thus

2𝑑2 + 3𝑑 βˆ’ 2 2𝑑 βˆ’ 1 = lim = βˆ’5. π‘‘β†’βˆ’2 𝑑2 + 5𝑑 + 6 π‘‘β†’βˆ’2 𝑑 + 3 lim

11. Factoring the numerator and the denominator and simplifying, we get (π‘₯ βˆ’ 3)(π‘₯ + 3) π‘₯+3 π‘₯2 βˆ’ 9 = = (π‘₯ βˆ’ 3)(π‘₯ + 4) π‘₯+4 π‘₯2 + π‘₯ βˆ’ 12 provided π‘₯ β‰  3. Thus lim

π‘₯2 βˆ’ 9

π‘₯β†’3 π‘₯2 + π‘₯ βˆ’ 12

= lim

π‘₯+3

π‘₯β†’3 π‘₯ + 4

=

6 . 7

12. Factoring the numerator and the denominator, we obtain (2𝑦 βˆ’ 1)(𝑦 + 1) 2𝑦 βˆ’ 1 2𝑦2 + 𝑦 βˆ’ 1 = = (3𝑦 βˆ’ 1)(𝑦 + 1) 3𝑦 βˆ’ 1 3𝑦2 + 2𝑦 βˆ’ 1 provided 𝑦 β‰  βˆ’1. Thus

2𝑦2 + 𝑦 βˆ’ 1 2𝑦 βˆ’ 1 3 = lim = . π‘¦β†’βˆ’1 3𝑦2 + 2𝑦 βˆ’ 1 π‘¦β†’βˆ’1 3𝑦 βˆ’ 1 4 lim

13. Expanding the numerator, we get

(3 + β„Ž)2 βˆ’ 9 = 9 + 6β„Ž + β„Ž2 βˆ’ 9 = 6β„Ž + β„Ž2 .

Next, factoring and simplifying, we get β„Ž(6 + β„Ž) (3 + β„Ž)2 βˆ’ 9 = =6+β„Ž β„Ž β„Ž provided β„Ž β‰  0. Thus

(3 + β„Ž)2 βˆ’ 9 = lim(6 + β„Ž) = 6. β„Žβ†’0 β„Žβ†’0 β„Ž lim

109


110

Chapter One /SOLUTIONS

14. Simplifying and factoring the numerator and the denominator, we obtain (π‘₯ + 3)(π‘₯ + 7) (π‘₯ + 5)2 βˆ’ 4 π‘₯2 + 10π‘₯ + 21 π‘₯+7 = = = 2 (π‘₯ + 3)(π‘₯ βˆ’ 3) π‘₯βˆ’3 π‘₯ βˆ’9 π‘₯2 βˆ’ 9 provided π‘₯ β‰  βˆ’3. Thus lim

π‘₯β†’βˆ’3

(π‘₯ + 5)2 βˆ’ 4 2 π‘₯+7 = lim =βˆ’ . π‘₯β†’βˆ’3 π‘₯ βˆ’ 3 3 π‘₯2 βˆ’ 9

15. Factoring the numerator and the denominator, we obtain 5(π‘₯2 βˆ’ 3) 5 5π‘₯2 βˆ’ 15 = 2 = 2 4 π‘₯ βˆ’9 (π‘₯ βˆ’ 3)(π‘₯2 + 3) π‘₯ +3 provided π‘₯ β‰ 

√

3. Thus

5 5π‘₯2 βˆ’ 15 5 = lim = . √ 4 2 6 π‘₯β†’ 3 π‘₯ βˆ’ 9 π‘₯β†’ 3 π‘₯ + 3 lim √

16. Rewriting the numerator as a single quotient we get 2βˆ•π‘₯ βˆ’ 1 = (2 βˆ’ π‘₯)βˆ•π‘₯. Then (2 βˆ’ π‘₯)βˆ•π‘₯ 2βˆ•π‘₯ βˆ’ 1 1 = =βˆ’ π‘₯βˆ’2 π‘₯βˆ’2 π‘₯ provided π‘₯ β‰  2. Thus lim π‘₯β†’2

17. Simplifying, we obtain

2βˆ•π‘₯ βˆ’ 1 1 1 = lim βˆ’ = βˆ’ . π‘₯β†’2 π‘₯ π‘₯βˆ’2 2

3βˆ’π‘‘

1βˆ•π‘‘ βˆ’ 1βˆ•3 βˆ’(𝑑 βˆ’ 3) 3βˆ’π‘‘ 1 βˆ’1 = 3𝑑 = β‹… = = π‘‘βˆ’3 π‘‘βˆ’3 3𝑑 π‘‘βˆ’3 3𝑑(𝑑 βˆ’ 3) 3𝑑 provided 𝑑 β‰  3. Thus lim 𝑑→3

1βˆ•π‘‘ βˆ’ 1βˆ•3 1 βˆ’1 = lim =βˆ’ . 𝑑→3 3𝑑 π‘‘βˆ’3 9

18. Rewriting the numerator as a single quotient, we have 1 βˆ’ (𝑑 + 1) 1 𝑑 βˆ’1= =βˆ’ 𝑑+1 𝑑+1 𝑑+1 Then

1βˆ•(𝑑 + 1) βˆ’ 1 π‘‘βˆ•(𝑑 + 1) 1 =βˆ’ =βˆ’ 𝑑 𝑑 𝑑+1

provided 𝑑 β‰  0. Thus

lim 𝑑→0

1βˆ•(𝑑 + 1) βˆ’ 1 1 = lim βˆ’ = βˆ’1. 𝑑→0 𝑑 𝑑+1

19. Rewriting the numerator as a single quotient we get 4 βˆ’ (4 + β„Ž) 1 1 4 4+β„Ž βˆ’β„Ž βˆ’ = βˆ’ = = 4+β„Ž 4 4(4 + β„Ž) 4(4 + β„Ž) 4(4 + β„Ž) 4(4 + β„Ž) provided β„Ž β‰  0. Thus lim

β„Žβ†’0

1βˆ•(4 + β„Ž) βˆ’ 1βˆ•4 1 βˆ’β„Ž βˆ’1 = lim == lim =βˆ’ . β„Žβ†’0 4β„Ž(4 + β„Ž) β„Žβ†’0 4(4 + β„Ž) β„Ž 16


1.9 SOLUTIONS 20. There are two ways to do this. One way is to multiply the numerator and denominator by

√

111

𝑧 + 1 and then simplify:

√ √ √ ( 𝑧)2 βˆ’ 1 ( 𝑧 βˆ’ 1)( 𝑧 + 1) 1 = = √ √ √ (𝑧 βˆ’ 1)( 𝑧 + 1) (𝑧 βˆ’ 1)( 𝑧 + 1) 𝑧+1 provided 𝑧 β‰  1. Thus

√ lim

A second way is to let 𝑒 =

π‘§βˆ’1

π‘§βˆ’1

𝑧→1

1 1 = . = lim √ 𝑧→1 2 𝑧+1

√ 𝑧 so 𝑧 = 𝑒2 . Since 𝑒 β†’ 1 as 𝑧 β†’ 1, we can rewrite √ lim 𝑧→1

π‘§βˆ’1

π‘§βˆ’1

= lim

π‘’βˆ’1

.

𝑒→1 𝑒2 βˆ’ 1

Factoring 𝑒2 βˆ’ 1 = (𝑒 βˆ’ 1)(𝑒 + 1) and canceling the 𝑒 βˆ’ 1 factors since 𝑒 β‰  1 in the limit, we get lim

π‘’βˆ’1

𝑒→1 𝑒2 βˆ’ 1

= lim

1

𝑒→1 𝑒 + 1

=

1 . 2

√ 21. There are two ways to do this. One way is to multiply the numerator and denominator by 9 + β„Ž + 3 and then simplify: (√ ) (√ ) 9+β„Žβˆ’3 9+β„Ž+3 9+β„Žβˆ’9 β„Ž 1 = (√ (√ ) ) = (√ ) = √ 9+β„Ž+3 β„Ž 9+β„Ž+3 β„Ž 9+β„Ž+3 β„Ž 9+β„Ž+3 provided β„Ž β‰  0. Thus

√ lim

β„Žβ†’0

A second way is to let 𝑒 =

√

9+β„Žβˆ’3 1 1 = . = lim √ β„Žβ†’0 β„Ž 6 9+β„Ž+3

9 + β„Ž so β„Ž = 𝑒2 βˆ’ 9. Since 𝑒 β†’ 3 as β„Ž β†’ 0, we can rewrite √ 9+β„Žβˆ’3 π‘’βˆ’3 . = lim 2 lim β„Žβ†’0 𝑒→3 𝑒 βˆ’ 9 β„Ž

Factoring 𝑒2 βˆ’ 9 = (𝑒 βˆ’ 3)(𝑒 + 3) and canceling the 𝑒 βˆ’ 3 factors since 𝑒 β‰  3 in the limit, we get lim

π‘’βˆ’3

𝑒→3 𝑒2 βˆ’ 9

= lim

1

𝑒→3 𝑒 + 3

=

1 . 6

22. There are two ways to do this. First, factoring the numerator and simplifying, we get (2π‘₯ )2 βˆ’ 1 (2π‘₯ βˆ’ 1)(2π‘₯ + 1) 4π‘₯ βˆ’ 1 = π‘₯ = = 2π‘₯ + 1 π‘₯ 2 βˆ’1 2 βˆ’1 2π‘₯ βˆ’ 1 provided π‘₯ β‰  0. Thus lim

4π‘₯ βˆ’ 1

π‘₯β†’0 2π‘₯ βˆ’ 1

= lim(2π‘₯ + 1) = 20 + 1 = 2. π‘₯β†’0

π‘₯

A second way is to let 𝑒 = 2 . Since 𝑒 β†’ 1 as π‘₯ β†’ 0, we can rewrite 4π‘₯ βˆ’ 1 𝑒2 βˆ’ 1 = lim . π‘₯ π‘₯β†’0 2 βˆ’ 1 𝑒→1 𝑒 βˆ’ 1

lim

Factoring 𝑒2 βˆ’ 1 = (𝑒 βˆ’ 1)(𝑒 + 1) and canceling the 𝑒 βˆ’ 1 factors since 𝑒 β‰  1 in the limit, we get 𝑒2 βˆ’ 1 = lim(𝑒 + 1) = 2. 𝑒→1 𝑒 βˆ’ 1 𝑒→1

lim


112

Chapter One /SOLUTIONS

23. Expanding the numerator, we get (1 + β„Ž)4 βˆ’ 1 = 1 + 4β„Ž + 6β„Ž2 + 4β„Ž3 + β„Ž4 βˆ’ 1. Next, factoring and simplifying, we get β„Ž(4 + 6β„Ž + 4β„Ž2 + β„Ž3 ) (1 + β„Ž)4 βˆ’ 1 = = 4 + 6β„Ž + 4β„Ž2 + β„Ž3 β„Ž β„Ž provided β„Ž β‰  0. Thus

(1 + β„Ž)4 βˆ’ 1 = lim(4 + 6β„Ž + 4β„Ž2 + β„Ž3 ) = 4. β„Žβ†’0 β„Žβ†’0 β„Ž lim

24. (a) We have 𝑓 (4) = 7 and 𝑔(4) = 4βˆ’2 , so the limit is of the form 7βˆ•(4βˆ’2 ), not 0βˆ•0. (b) Since 𝑓 (π‘₯)βˆ•π‘”(π‘₯) is continuous at 𝑐 = 4, we have lim

𝑓 (π‘₯)

π‘₯β†’4 𝑔(π‘₯)

=

𝑓 (4) 7 = βˆ’2 = 7 β‹… 16 = 112. 𝑔(4) 4

25. (a) We have 𝑓 (1) = 2(1)3 + (1)2 βˆ’ 3(1) = 0 and 𝑔(1) = (1)2 + 3(1) βˆ’ 4 = 0, so the limit is of the form 0βˆ•0. (b) Factoring, we have lim π‘₯β†’1

So lim π‘₯β†’1

π‘₯(2π‘₯2 + π‘₯ βˆ’ 3) 2π‘₯3 + π‘₯2 βˆ’ 3π‘₯ = lim π‘₯β†’1 (π‘₯ βˆ’ 1)(π‘₯ + 4) π‘₯2 + 3π‘₯ βˆ’ 4 π‘₯(2π‘₯ + 3)(π‘₯ βˆ’ 1) = lim π‘₯β†’1 (π‘₯ βˆ’ 1)(π‘₯ + 4) π‘₯(2π‘₯ + 3) = lim π‘₯β†’1 (π‘₯ + 4) (1)(2(1) + 3) 5 = = 1. = lim π‘₯β†’1 (1 + 4) 5

2π‘₯3 + π‘₯2 βˆ’ 3π‘₯ = 1. π‘₯2 + 3π‘₯ βˆ’ 4

26. (a) We have 𝑓 (3) = (3)2 βˆ’ 3(3) = 0 and 𝑔(3) = (b) Rationalizing the denominator, we have

√ 3 + 1 βˆ’ 2 = 0, so the limit is of the form 0βˆ•0.

√ π‘₯+1+2 π‘₯2 βˆ’ 3π‘₯ π‘₯2 βˆ’ 3π‘₯ = lim √ β‹…βˆš lim √ π‘₯β†’3 π‘₯β†’3 π‘₯+1βˆ’2 π‘₯+1βˆ’2 π‘₯+1+2 √ (π‘₯2 βˆ’ 3π‘₯)( π‘₯ + 1 + 2) = lim π‘₯β†’3 (π‘₯ + 1) βˆ’ 4 √ π‘₯(π‘₯ βˆ’ 3)( π‘₯ + 1 + 2) = lim π‘₯β†’3 (π‘₯ βˆ’ 3) √ = lim π‘₯( π‘₯ + 1 + 2) π‘₯β†’3 √ = 3( 3 + 1 + 2) = 3(2 + 2) = 12. π‘₯2 βˆ’ 3π‘₯ = 12. So lim √ π‘₯β†’3 π‘₯+1βˆ’2 27. Dividing both numerator and denominator by 𝑧3 , we get 5 + 𝑧22 + 𝑧13 0+0+0 5𝑧2 + 2𝑧 + 1 𝑧 = lim = = 0. π‘§β†’βˆž 2𝑧3 βˆ’ 𝑧2 + 9 π‘§β†’βˆž 2 βˆ’ 1 + 9 2βˆ’0+0

lim

𝑧

𝑧3

28. Dividing both numerator and denominator by π‘₯2 , we get 1 + 7 βˆ’ π‘₯112 7 π‘₯ + 7π‘₯2 βˆ’ 11 π‘₯ = lim = . 2 π‘₯β†’βˆž π‘₯β†’βˆž 3 3π‘₯2 βˆ’ 2π‘₯ 3βˆ’

lim

π‘₯


1.9 SOLUTIONS 29. Dividing both numerator and denominator by 𝑒𝑑 , we get 4 + 𝑒32𝑑 4 4𝑒𝑑 + 3π‘’βˆ’π‘‘ = . = lim π‘‘β†’βˆž 5𝑒𝑑 + 2𝑒 π‘‘β†’βˆž 5 + 2𝑒 5 lim

𝑒𝑑

30. We have,

( )π‘₯ 2π‘₯+1 2π‘₯ β‹… 2 2 = lim = lim 6 =0 π‘₯β†’βˆž 3π‘₯βˆ’1 π‘₯β†’βˆž 3π‘₯ β‹… 3βˆ’1 π‘₯β†’βˆž 3 π‘₯ since lim (2βˆ•3) = 0 because 2βˆ•3 < 1. lim

π‘₯β†’βˆž

31. We have,

23π‘₯+2 23π‘₯ β‹… 22 = lim π‘₯ 3 = lim π‘₯+3 π‘₯β†’βˆž 3 π‘₯β†’βˆž 3 β‹… 3 π‘₯β†’βˆž lim

( )π‘₯ 8 = ∞ because 83 > 1. π‘₯β†’βˆž 3 32. We have,

( 3 )π‘₯ ( ) ( )π‘₯ ( ) 2 4 8 4 = lim = ∞, π‘₯β†’βˆž 3 3 27 27

since lim

lim π‘₯π‘’βˆ’π‘₯ = lim

π‘₯β†’βˆž π‘₯

since 𝑒 grows faster than π‘₯.

π‘₯

π‘₯β†’βˆž 𝑒π‘₯

33. We have,

= 0,

lim (4𝑒𝑑 )(7π‘’βˆ’π‘‘ ) = lim

28𝑒𝑑 = 28. 𝑒𝑑

lim π‘‘βˆ’2 sin 𝑑 = lim

sin 𝑑 = 0, 𝑑2

π‘‘β†’βˆž

π‘‘β†’βˆž

34. We have, π‘‘β†’βˆž

π‘‘β†’βˆž

since βˆ’1 ≀ sin 𝑑 ≀ 1 and 𝑑2 β†’ ∞ as 𝑑 β†’ ∞. (√ ) 35. First we use algebra: Multiply by 4 + β„Ž + 2 in numerator and denominator, then expand and simplify: √ 4+β„Žβˆ’2=

(√

) (√ ) 4+β„Žβˆ’2 4+β„Ž+2 β„Ž 4+β„Žβˆ’4 = √ . = √ (√ ) 4+β„Ž+2 4+β„Ž+2 4+β„Ž+2

Now we can find the limit: √ lim

β„Žβ†’0

36. First we combine the fractions:

4+β„Žβˆ’2 1 β„Ž 1 = . = lim (√ ) = lim √ β„Žβ†’0 β„Žβ†’0 β„Ž 4 4+β„Ž+2 β„Ž 4+β„Ž+2 √ 2βˆ’ 4+β„Ž 1 βˆ’ = √ . √ 2 4+β„Ž 4+β„Ž 2 1

Now multiply by

(√ ) 4 + β„Ž + 2 in numerator and denominator, then expand and simplify:

(

)( ) √ √ 2βˆ’ 4+β„Ž 2+ 4+β„Ž 4 βˆ’ (4 + β„Ž) βˆ’β„Ž = √ ( ) ( ) = √ ( ). √ √ √ √ 2 4+β„Ž 2+ 4+β„Ž 2 4+β„Ž 2+ 4+β„Ž 2 4+β„Ž 2+ 4+β„Ž

Now we find the limit: ( ) 1 1 1 βˆ’β„Ž βˆ’1 1 βˆ’ = lim √ lim ( ) = lim √ ( ) =βˆ’ . √ √ √ β„Žβ†’0 β„Ž β„Žβ†’0 β„Žβ†’0 16 4+β„Ž 2 2β„Ž 4 + β„Ž 2 + 4 + β„Ž 2 4+β„Ž 2+ 4+β„Ž

113


114

Chapter One /SOLUTIONS

37. Given that βˆ’4π‘₯ + 6 ≀ 𝑓 (π‘₯) ≀ π‘₯2 βˆ’ 2π‘₯ + 7, we see that lim (βˆ’4π‘₯ + 6) ≀ lim 𝑓 (π‘₯) ≀ lim (π‘₯2 βˆ’ 2π‘₯ + 7)

π‘₯β†’βˆ’1

π‘₯β†’βˆ’1

π‘₯β†’βˆ’1

βˆ’4(βˆ’1) + 6 ≀ lim 𝑓 (π‘₯) ≀ (βˆ’1)2 βˆ’ 2(βˆ’1) + 7 π‘₯β†’βˆ’1

10 ≀ lim 𝑓 (π‘₯) ≀ 10. π‘₯β†’βˆ’1

Since 10 ≀ lim 𝑓 (π‘₯) ≀ 10, we know that lim 𝑓 (π‘₯) = 10. π‘₯β†’βˆ’1

π‘₯β†’βˆ’1

38. Given that 4 cos(2π‘₯) ≀ 𝑓 (π‘₯) ≀ 3π‘₯2 + 4, we see that lim 4 cos(2π‘₯) ≀ lim 𝑓 (π‘₯) ≀ lim(3π‘₯2 + 4) π‘₯β†’0

π‘₯β†’0

π‘₯β†’0

4 cos(0) ≀ lim 𝑓 (π‘₯) ≀ 3(0)2 + 4 π‘₯β†’0

4 ≀ lim 𝑓 (π‘₯) ≀ 4. π‘₯β†’0

Since 4 ≀ lim 𝑓 (π‘₯) ≀ 4, we know that lim 𝑓 (π‘₯) = 4. π‘₯β†’0

π‘₯β†’0

4π‘₯2 βˆ’ 5 4π‘₯6 + 3 39. Given that ≀ 𝑓 (π‘₯) ≀ , we see that π‘₯2 π‘₯6 4π‘₯2 βˆ’ 5 4π‘₯6 + 3 ≀ lim 𝑓 (π‘₯) ≀ lim 2 π‘₯β†’βˆž π‘₯β†’βˆž π‘₯ π‘₯6 4π‘₯2 5 4π‘₯6 3 lim βˆ’ lim 2 ≀ lim 𝑓 (π‘₯) ≀ lim 6 + lim 6 π‘₯β†’βˆž π‘₯2 π‘₯β†’βˆž π‘₯ π‘₯β†’βˆž π‘₯β†’βˆž π‘₯ π‘₯β†’βˆž π‘₯ (using the sum property since each limit exists) lim

π‘₯β†’βˆž

4 βˆ’ 0 ≀ lim 𝑓 (π‘₯) ≀ 4 + 0 π‘₯β†’βˆž

4 ≀ lim 𝑓 (π‘₯) ≀ 4. π‘₯β†’βˆž

Since 4 ≀ lim 𝑓 (π‘₯) ≀ 4, we know that lim 𝑓 (π‘₯) = 4. π‘₯β†’βˆž

π‘₯β†’βˆž

PROBLEMS 40. Because the denominator equals 0 when π‘₯ = 4, so must the numerator. This means π‘˜2 = 16 and the choices for π‘˜ are 4 or βˆ’4. 41. Because the denominator equals 0 when π‘₯ = 1, so must the numerator. So 1 βˆ’ π‘˜ + 4 = 0. The only possible value of π‘˜ is 5. 42. Because the denominator equals 0 when π‘₯ = βˆ’2, so must the numerator. So 4 βˆ’ 8 + π‘˜ = 0 and the only possible value of π‘˜ is 4. 43. Because the denominator equals 0 when π‘₯ = 5, so must the numerator. So 25 βˆ’ 5π‘˜ + 5 = 0 and the only possible value of π‘˜ is 6. 44. Because the denominator equals 0 when π‘₯ = 0, so must the numerator. So π‘’π‘˜ βˆ’ 8 = 0 and the only possible value of π‘˜ is ln 8. 45. Because the denominator equals 0 when π‘₯ = 1, so must the numerator. So π‘˜2 βˆ’ 49 = 0 and the choices for π‘˜ are 7 or βˆ’7. 46. Division of numerator and denominator by π‘₯2 yields 1 + 3βˆ•π‘₯ + 5βˆ•π‘₯2 π‘₯2 + 3π‘₯ + 5 = . π‘˜ 4π‘₯ + 1 + π‘₯ 4βˆ•π‘₯ + 1βˆ•π‘₯2 + π‘₯π‘˜βˆ’2 As π‘₯ β†’ ∞, the limit of the numerator is 1. The limit of the denominator depends upon π‘˜. If π‘˜ > 2, the denominator approaches ∞ as π‘₯ β†’ ∞, so the limit of the quotient is 0. If π‘˜ = 2, the denominator approaches 1 as π‘₯ β†’ ∞, so the limit of the quotient is 1. If π‘˜ < 2 the denominator approaches 0+ as π‘₯ β†’ ∞, so the limit of the quotient is ∞. Therefore the values of π‘˜ we are looking for are π‘˜ β‰₯ 2.


1.9 SOLUTIONS

115

) ) ( ( 47. For the numerator, lim 𝑒2π‘₯ βˆ’ 5 = βˆ’5. If π‘˜ > 0, lim π‘’π‘˜π‘₯ + 3 = 3, so the quotient has a limit of βˆ’5βˆ•3. If π‘˜ = 0, π‘₯β†’βˆ’βˆž π‘₯β†’βˆ’βˆž ) ( lim π‘’π‘˜π‘₯ + 3 = 4, so the quotient has limit of βˆ’5βˆ•4. If π‘˜ < 0, the limit of the quotient is given by lim (𝑒2π‘₯ βˆ’5)βˆ•(π‘’π‘˜π‘₯ +3) = π‘₯β†’βˆ’βˆž

π‘₯β†’βˆ’βˆž

0.

48. Division of numerator and denominator by π‘₯3 yields 1 βˆ’ 6βˆ•π‘₯3 π‘₯3 βˆ’ 6 . = π‘˜βˆ’3 π‘₯π‘˜ + 3 π‘₯ + 3βˆ•π‘₯3 As π‘₯ β†’ ∞, the limit of the numerator is 1. The limit of the denominator depends upon π‘˜. If π‘˜ > 3, the denominator approaches ∞ as π‘₯ β†’ ∞, so the limit of the quotient is 0. If π‘˜ = 3, the denominator approaches 1 as π‘₯ β†’ ∞, so the limit of the quotient is 1. If π‘˜ < 3 the denominator approaches 0+ as π‘₯ β†’ ∞, so the limit of the quotient is ∞. Therefore the values of π‘˜ we are looking for are π‘˜ β‰₯ 3. 49. We divide both the numerator and denominator by 𝑒5π‘₯ , giving 𝑒(π‘˜βˆ’5)π‘₯ + 11βˆ•π‘’5π‘₯ π‘’π‘˜π‘₯ + 11 = lim . π‘₯β†’βˆž 𝑒5π‘₯ βˆ’ 3 π‘₯β†’βˆž 1 βˆ’ 3βˆ•π‘’5π‘₯ lim

In the denominator, lim 1 βˆ’ 3βˆ•π‘’5π‘₯ = 1. In the numerator, if π‘˜ < 5, we have lim (𝑒(π‘˜βˆ’5)π‘₯ + 11βˆ•π‘’5π‘₯ ) = 0, so the quotient π‘₯β†’βˆž

π‘₯β†’βˆž

has a limit of 0. If π‘˜ = 5, we have lim (𝑒(π‘˜βˆ’5)π‘₯ + 11βˆ•π‘’5π‘₯ ) = 1, so the quotient has a limit of 1. If π‘˜ > 5, we have π‘₯β†’βˆž

lim (𝑒(π‘˜βˆ’5)π‘₯ + 11βˆ•π‘’5π‘₯ ) = ∞, so the limit of the quotient does not exist.

π‘₯β†’βˆž

50. We divide both the numerator and denominator by 32π‘₯ , giving 3(π‘˜βˆ’2)π‘₯ + 6βˆ•32π‘₯ 3π‘˜π‘₯ + 6 = . 2π‘₯ π‘₯β†’βˆž 3 + 4 1 + 4βˆ•32π‘₯ lim

In the denominator, lim 1+4βˆ•32π‘₯ = 1. In the numerator, if π‘˜ < 2, we have lim 3(π‘˜βˆ’2)π‘₯ +6βˆ•32π‘₯ = 0, so the quotient has a limit π‘₯β†’βˆž

π‘₯β†’βˆž

of 0. If π‘˜ = 2, we have lim 3(π‘˜βˆ’2)π‘₯ + 6βˆ•32π‘₯ = 1, so the quotient has a limit of 1. If π‘˜ > 2, we have lim 3(π‘˜βˆ’2)π‘₯ + 6βˆ•32π‘₯ = ∞, π‘₯β†’βˆž π‘₯β†’βˆž so the quotient has a limit of ∞. 51. In the denominator, we have lim 32π‘₯ + 4 = 4. In the numerator, if π‘˜ < 0, we have lim 3π‘˜π‘₯ + 6 = ∞, so the quotient has π‘₯β†’βˆ’βˆž

π‘₯β†’βˆ’βˆž

a limit of ∞. If π‘˜ = 0, we have lim 3π‘˜π‘₯ + 6 = 7, so the quotient has a limit of 7βˆ•4. If π‘˜ > 0, we have lim 3π‘˜π‘₯ + 6 = 6, π‘₯β†’βˆ’βˆž

π‘₯β†’βˆ’βˆž

so the quotient has a limit of 6βˆ•4. √ 52. Let 𝑑 = 𝑦 so that 𝑦 = 𝑑2 . Since 𝑑 β†’ 2 as 𝑦 β†’ 4, we have lim 𝑦→4

53. Let 𝑑 =

√

√ π‘¦βˆ’2 π‘¦βˆ’4

π‘‘βˆ’2 = lim 2 𝑑→2 𝑑 βˆ’ 4 π‘‘βˆ’2 = lim 𝑑→2 (𝑑 βˆ’ 2)(𝑑 + 2) 1 = lim 𝑑→2 𝑑 + 2 1 = . 4

π‘₯ so that π‘₯ = 𝑑2 . Since 𝑑 β†’ 3 as π‘₯ β†’ 9, we have √ π‘₯βˆ’ π‘₯βˆ’6 𝑑2 βˆ’ 𝑑 βˆ’ 6 = lim lim √ π‘₯β†’9 𝑑→3 π‘‘βˆ’3 π‘₯βˆ’3 (𝑑 βˆ’ 3)(𝑑 + 2) = lim 𝑑→3 π‘‘βˆ’3 = lim(𝑑 + 2) 𝑑→3

= 5.


116

Chapter One /SOLUTIONS

54. Let 𝑑 =

√

1 + β„Ž so that 𝑑2 = 1 + β„Ž and β„Ž = 𝑑2 βˆ’ 1. Since 𝑑 β†’ 1 as β„Ž β†’ 0, we have √ 1+β„Žβˆ’1 π‘‘βˆ’1 lim = lim 2 β„Žβ†’0 𝑑→1 𝑑 βˆ’ 1 β„Ž π‘‘βˆ’1 = lim 𝑑→1 (𝑑 βˆ’ 1)(𝑑 + 1) 1 = lim 𝑑→1 𝑑 + 1 1 = . 2

√ 55. Let 𝑑 = 3 π‘₯ so that π‘₯ = 𝑑3 . Since 𝑑 β†’ 1 as π‘₯ β†’ 1, we have √ 3 π‘₯βˆ’1 π‘‘βˆ’1 lim = lim 3 π‘₯β†’1 π‘₯ βˆ’ 1 𝑑→1 𝑑 βˆ’ 1 = lim

π‘‘βˆ’1

𝑑→1 (𝑑 βˆ’ 1)(𝑑2 + 𝑑 + 1)

1 = lim 2 𝑑→1 𝑑 + 𝑑 + 1 1 = . 3 56. Let 𝑑 = 𝑒π‘₯ so that 𝑒3π‘₯ = (𝑒π‘₯ )3 = 𝑑3 and 𝑒2π‘₯ = 𝑑2 . Since 𝑑 β†’ 1 as π‘₯ β†’ 0, we have 𝑒3π‘₯ βˆ’ 𝑒2π‘₯ 𝑑3 βˆ’ 𝑑2 = lim π‘₯ π‘₯β†’0 𝑒 βˆ’ 1 𝑑→1 𝑑 βˆ’ 1 𝑑2 (𝑑 βˆ’ 1) = lim 𝑑→1 π‘‘βˆ’1 = lim 𝑑2

lim

𝑑→1

= 1. 57. Let 𝑑 = 𝑒π‘₯ so that 𝑒3π‘₯ = (𝑒π‘₯ )3 = 𝑑3 . Since 𝑑 β†’ ∞ as π‘₯ β†’ ∞, we have: lim

2𝑒3π‘₯ βˆ’ 1

π‘₯β†’βˆž 5𝑒3π‘₯ + 𝑒π‘₯ + 1

= lim

2𝑑3 βˆ’ 1

π‘‘β†’βˆž 5𝑑3 + 𝑑 + 1

2 βˆ’ 1βˆ•π‘‘3 Dividing numerator and denominator by 𝑑3 π‘‘β†’βˆž 5 + π‘‘βˆ•π‘‘3 + 1βˆ•π‘‘3 2 βˆ’ 1βˆ•π‘‘3 = lim Simplifying π‘‘β†’βˆž 5 + 1βˆ•π‘‘2 + 1βˆ•π‘‘3 2βˆ’0 2 = Since 1βˆ•π‘‘2 β†’ 0 and 1βˆ•π‘‘3 β†’ 0 as 𝑑 β†’ ∞ = . 5+0+0 5 = lim

1 sin π‘₯ 1 ≀ ≀ . Since π‘₯ π‘₯ π‘₯ 1 1 lim βˆ’ = 0 = lim , π‘₯β†’βˆž π‘₯ π‘₯β†’βˆž π‘₯

58. We know that βˆ’1 ≀ sin π‘₯ ≀ 1. If we divide by π‘₯, π‘₯ β‰  0, we get βˆ’

we know that lim

π‘₯β†’βˆž

sin π‘₯ = 0. π‘₯

59. For π‘₯ β‰₯ 0, since 0 < π‘’βˆ’π‘₯ ≀ 1, we have π‘₯ < π‘₯ + π‘’βˆ’π‘₯ < π‘₯ + 1. Therefore, lim

1

π‘₯β†’βˆž π‘₯ + 1

= 0 = lim

1

π‘₯β†’βˆž π‘₯

, we have lim

1

π‘₯β†’βˆž π‘₯ + 1

≀ lim

1

π‘₯β†’βˆž π‘₯ + π‘’βˆ’π‘₯

0 ≀ lim

1

π‘₯β†’βˆž π‘₯ + π‘’βˆ’π‘₯

≀ lim

1

π‘₯β†’βˆž π‘₯

≀0

1 1 1 < . Therefore, since < π‘₯+1 π‘₯ + π‘’βˆ’π‘₯ π‘₯


1.9 SOLUTIONS 1

Thus, lim

π‘₯β†’βˆž π‘₯ + π‘’βˆ’π‘₯

= 0.

60. For all π‘₯, we know that βˆ’1 ≀ cos π‘₯ ≀ 1, and hence that 0 ≀ cos2 π‘₯ ≀ 1. It follows that 1 cos2 π‘₯ ≀ . 2π‘₯ + 1 2π‘₯ + 1

0≀ Therefore, since lim 0 = 0 and lim

1

π‘₯β†’βˆž 2π‘₯ + 1

π‘₯β†’βˆž

= 0, we have lim

cos2 π‘₯

π‘₯β†’βˆž 2π‘₯ + 1

= 0 by the Squeeze Theorem.

61. For all π‘₯ β‰  0, we know that βˆ’1 ≀ sin(1βˆ•π‘₯) ≀ 1. It follows that βˆ’π‘₯4 ≀ π‘₯4 sin(1βˆ•π‘₯) ≀ π‘₯4 . Therefore, since lim(βˆ’π‘₯4 ) = 0 and lim π‘₯4 = 0, we have lim π‘₯4 sin(1βˆ•π‘₯) = 0 by the Squeeze Theorem. π‘₯β†’0

π‘₯β†’0

π‘₯β†’0

62. For all π‘₯ β‰₯ 0, we know that

π‘₯ 1 π‘₯ 0≀ √ ≀ √ = √ . 3 3 π‘₯ π‘₯ +1 π‘₯ 1 π‘₯ Therefore, since lim 0 = 0 and lim √ = 0, we have lim √ = 0 by the Squeeze Theorem. π‘₯β†’βˆž π‘₯β†’βˆž π‘₯β†’βˆž π‘₯ π‘₯3 + 1 63. We know that βˆ’1 ≀ cos π‘₯ ≀ 1, and hence that 0 ≀ 2 cos2 π‘₯ ≀ 2. Therefore, π‘₯ ≀ π‘₯ + 2 cos2 π‘₯ ≀ π‘₯ + 2, so for π‘₯ > 0, 1 1 1 ≀ . ≀ π‘₯+2 π‘₯ π‘₯ + 2 cos2 π‘₯ 1

Since lim

π‘₯β†’βˆž π‘₯ + 2

64. Since π‘₯2 sin

( ) 1 π‘₯

= 0 and lim

1

π‘₯β†’βˆž π‘₯

1

= 0, we have lim

π‘₯β†’βˆž π‘₯ + 2 cos2 π‘₯

= 0 by the Squeeze Theorem.

+ 1 is squeezed between 𝑦 = π‘₯2 + 1 and 𝑦 = βˆ’π‘₯2 + 1, ) ( ( ) 1 + 1 = lim(π‘₯2 + 1) = lim(βˆ’π‘₯2 + 1) = 1. lim π‘₯2 sin π‘₯β†’0 π‘₯β†’0 π‘₯β†’0 π‘₯

See Figure 1.127. 𝑦 𝑦 = π‘₯2 + 1 𝑦 = π‘₯2 sin

( ) 1 π‘₯

+1

𝑦 = βˆ’π‘₯2 + 1 π‘₯

Figure 1.127

65. Since sin

( ) 1 π‘₯

+ 2 is oscillates between 𝑦 = 3 and 𝑦 = 1, the limit as π‘₯ β†’ 0 does not exist. See Figure 1.128. 𝑦 𝑦=3 ( ) 𝑦 = sin π‘₯1 + 2 𝑦=1 π‘₯

Figure 1.128

117


118

Chapter One /SOLUTIONS

66. There are many possible correct answers. (a) If 𝑓 (π‘₯) = 1βˆ•π‘₯2 and 𝑔(π‘₯) = 1βˆ•π‘₯ then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 1βˆ•π‘₯ so lim

𝑓 (π‘₯)

π‘₯β†’βˆž 𝑔(π‘₯)

= 0.

𝑓 (π‘₯) = 1. (b) If 𝑓 (π‘₯) = 1βˆ•π‘₯ and 𝑔(π‘₯) = 1βˆ•π‘₯ then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 1 so lim π‘₯β†’βˆž 𝑔(π‘₯) 𝑓 (π‘₯) = ∞. (c) If 𝑓 (π‘₯) = 1βˆ•π‘₯ and 𝑔(π‘₯) = 1βˆ•π‘₯2 then 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = π‘₯ so lim π‘₯β†’βˆž 𝑔(π‘₯) 67. There are many possible choices for 𝑔(π‘₯). One possibility is 𝑔(π‘₯) =

(

) ( ) π‘₯3 βˆ’ 3π‘₯2 + π‘₯ βˆ’ 3 π‘₯βˆ’3 π‘₯βˆ’3 β‹… 𝑓 (π‘₯) = (π‘₯2 + 1) = . π‘₯βˆ’3 π‘₯βˆ’3 π‘₯βˆ’3

Observe that 𝑓 (π‘₯) = 𝑔(π‘₯) wherever 𝑓 (π‘₯) is defined except for π‘₯ = 3 since 𝑔(3) is undefined. This means the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) will be the same except at π‘₯ = 3 where the graph of 𝑔(π‘₯) has a hole. Since the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) are identical except at π‘₯ = 3, the hole will have the same coordinates as the function 𝑓 (π‘₯) at π‘₯ = 3, so the coordinates of the hole will be (3, 10). 68. There are many possible choices for 𝑔(π‘₯). One possibility is 𝑔(π‘₯) =

( ) ( ) π‘₯3 + π‘₯ π‘₯ π‘₯ β‹… 𝑓 (π‘₯) = (π‘₯2 + 1) = . π‘₯ π‘₯ π‘₯

Observe that 𝑓 (π‘₯) = 𝑔(π‘₯) wherever 𝑓 (π‘₯) is defined except for π‘₯ = 0 since 𝑔(0) is undefined. This means the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) will be the same except at π‘₯ = 0 where the graph of 𝑔(π‘₯) has a hole. Since the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) are identical except at π‘₯ = 0, the hole will have the same coordinates as the function 𝑓 (π‘₯) at π‘₯ = 0, so the coordinates of the hole will be (0, 1). 69. There are many possible choices for 𝑔(π‘₯). One possibility is ) ( ) ( π‘₯ ln π‘₯ βˆ’ ln π‘₯ π‘₯βˆ’1 π‘₯βˆ’1 β‹… 𝑓 (π‘₯) = ln π‘₯ = . 𝑔(π‘₯) = π‘₯βˆ’1 π‘₯βˆ’1 π‘₯βˆ’1 Observe that 𝑓 (π‘₯) = 𝑔(π‘₯) wherever 𝑓 (π‘₯) is defined except for π‘₯ = 1 since 𝑔(1) is undefined. This means the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) will be the same except at π‘₯ = 1 where the graph of 𝑔(π‘₯) has a hole. Since the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) are identical except at π‘₯ = 1, the hole will have the same coordinates as the function 𝑓 (π‘₯) at π‘₯ = 1, so the coordinates of the hole will be (1, 0). 70. There are many possible choices for 𝑔(π‘₯). One possibility is ) ( ) ( π‘₯ sin π‘₯ βˆ’ πœ‹ sin π‘₯ π‘₯βˆ’πœ‹ π‘₯βˆ’πœ‹ β‹… 𝑓 (π‘₯) = sin π‘₯ = . 𝑔(π‘₯) = π‘₯βˆ’πœ‹ π‘₯βˆ’πœ‹ π‘₯βˆ’πœ‹ Observe that 𝑓 (π‘₯) = 𝑔(π‘₯) wherever 𝑓 (π‘₯) is defined except for π‘₯ = πœ‹ since 𝑔(πœ‹) is undefined. This means the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) will be the same except at π‘₯ = πœ‹ where the graph of 𝑔(π‘₯) has a hole. Since the graphs of 𝑓 (π‘₯) and 𝑔(π‘₯) are identical except at π‘₯ = πœ‹, the hole will have the same coordinates as the function 𝑓 (π‘₯) at π‘₯ = πœ‹, so the coordinates of the hole will be (πœ‹, 0). 71. We have (π‘₯ βˆ’ 1)3 π‘₯β†’1 (π‘₯ βˆ’ 1)2 = lim(π‘₯ βˆ’ 1)

Cancelling (π‘₯ βˆ’ 1) since π‘₯ β‰  1

= 1 βˆ’ 1 = 0.

Substituting π‘₯ = 1 since (π‘₯ βˆ’ 1) is continuous

lim 𝑓 (π‘₯) = lim π‘₯β†’1

π‘₯β†’1

72. We have (π‘₯ βˆ’ 1)2 π‘₯β†’1 (π‘₯ βˆ’ 1)3 1 = lim π‘₯β†’1 (π‘₯ βˆ’ 1)

lim 𝑓 (π‘₯) = lim π‘₯β†’1

Cancelling (π‘₯ βˆ’ 1)2 since π‘₯ β‰  1

So the function 𝑓 (π‘₯) takes the same values as 1βˆ•(π‘₯ βˆ’ 1) except at π‘₯ = 1, so it must have the same limit. Since the limit of the denominator of 1βˆ•(π‘₯ βˆ’ 1) is 0 and the numerator is 1 at π‘₯ = 1, this limit does not exist.


1.9 SOLUTIONS

119

73. We have (π‘₯ βˆ’ 1)2 π‘₯β†’1 (π‘₯ βˆ’ 1)2 = lim(1) Cancelling (π‘₯ βˆ’ 1)2 since π‘₯ β‰  1

lim 𝑓 (π‘₯) = lim π‘₯β†’1

π‘₯β†’1

= 1. 74. We have lim 𝑓 (π‘₯) = lim π‘₯β†’1

(π‘₯ βˆ’ 1)𝑛

π‘₯β†’1 (π‘₯ βˆ’ 1)π‘š

= lim(π‘₯ βˆ’ 1)π‘›βˆ’π‘š

Cancelling (π‘₯ βˆ’ 1)π‘š since π‘₯ β‰  1 and 𝑛 > π‘š

π‘₯β†’1

= (1 βˆ’ 1)π‘›βˆ’π‘š = 0.

Substituting π‘₯ = 1 since (π‘₯ βˆ’ 1)π‘›βˆ’π‘š is continuous

75. We have (π‘₯ βˆ’ 1)𝑛 π‘₯β†’1 (π‘₯ βˆ’ 1)π‘š 1 = lim π‘₯β†’1 (π‘₯ βˆ’ 1)π‘šβˆ’π‘›

lim 𝑓 (π‘₯) = lim π‘₯β†’1

Cancelling (π‘₯ βˆ’ 1)𝑛 since π‘₯ β‰  1 and π‘š > 𝑛

So the function 𝑓 (π‘₯) takes the same values as 1βˆ•(π‘₯ βˆ’ 1)π‘šβˆ’π‘› except at π‘₯ = 1, so it must have the same limit. Since the limit of the denominator of 1βˆ•(π‘₯ βˆ’ 1)π‘šβˆ’π‘› is 0 and the numerator is 1 at π‘₯ = 1, this limit does not exist. 76. Since π‘š = 𝑛, we have lim 𝑓 (π‘₯) = lim π‘₯β†’1

(π‘₯ βˆ’ 1)𝑛

π‘₯β†’1 (π‘₯ βˆ’ 1)𝑛

= lim(1)

Cancelling (π‘₯ βˆ’ 1)𝑛 since π‘₯ β‰  1

π‘₯β†’1

= 1. 1 1 1 1 = 0 = lim and lim βˆ’ = 0 = lim . π‘₯β†’βˆž π‘₯ π‘₯β†’βˆ’βˆž π‘₯ π‘₯β†’βˆ’βˆž π‘₯ π‘₯ In both cases 𝐿 = 0. The Squeeze Theorem cannot be applied to other cases since for any other 𝑐,

77. The Squeeze Theorem can be applied when 𝑐 = ∞ or 𝑐 = βˆ’βˆž since lim βˆ’ π‘₯β†’βˆž

lim βˆ’ π‘₯→𝑐

1 1 1 1 = βˆ’ β‰  = lim . π‘₯ 𝑐 𝑐 π‘₯→𝑐 π‘₯

Strengthen Your Understanding 78. If we factor the numerator of 𝑓 and simplify, we see that 𝑓 (π‘₯) = π‘₯ βˆ’ 1, for π‘₯ β‰  βˆ’1. This show that the two functions are identical (that is, have the same values) where they are both defined, the functions have different domains: π‘₯ = βˆ’1 is in the domain of 𝑔 but not in the domain of 𝑓 . 79. The limit lim 𝑓 (π‘₯)βˆ•π‘”(π‘₯) depends on the values of 𝑓 (π‘₯)βˆ•π‘”(π‘₯) as π‘₯ approaches 1 but is not necessarily dependent on the π‘₯β†’1

value at π‘₯ = 1. For example, we can take 𝑔(π‘₯) = 1 and { 𝑓 (π‘₯) =

βˆ’1 0 1

π‘₯<1 π‘₯=1 . 1<π‘₯

For these choices of 𝑓 (π‘₯) and 𝑔(π‘₯), we have 𝑓 (1) = 0 and 𝑔(1) = 1 as required. However, for all π‘₯ < 1, 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = βˆ’1 so limβˆ’ 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = βˆ’1, and for π‘₯ > 1, 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 1, so lim+ 𝑓 (π‘₯)βˆ•π‘”(π‘₯) = 1. Thus the one sided limits are different, so π‘₯β†’1

lim 𝑓 (π‘₯)βˆ•π‘”(π‘₯) does not exist.

π‘₯β†’1

π‘₯β†’1

80. False, since the limit lim 𝑓 (π‘₯) may not even exist. For example if 𝑏(π‘₯) = βˆ’1, π‘Ž(π‘₯) = 1 and 𝑓 (π‘₯) = sin(1βˆ•π‘₯), then the π‘₯β†’0

conditions are met but sin(1βˆ•π‘₯) has no limit as π‘₯ β†’ 0. 81. True, by the Squeeze Theorem, using the constant function 𝑏(π‘₯) = 0.


120

Chapter One /SOLUTIONS

82. False, this is a confused, and incorrect, version of the Squeeze Theorem. For example if 𝑏(π‘₯) = 𝑓 (π‘₯) = π‘₯, and π‘Ž(π‘₯) = 1 then the conditions are met but lim 𝑓 (π‘₯) = 0 and lim π‘Ž(π‘₯) = 1. π‘₯β†’0

π‘₯β†’0

83. False, for example if 𝑓 (π‘₯) = 0, and 𝑔(π‘₯) = π‘₯ then the conditions are met but lim

𝑓 (π‘₯)

π‘₯β†’0 𝑔(π‘₯)

84. False, for example if 𝑓 (π‘₯) = 1, and 𝑔(π‘₯) = π‘₯ then the conditions are met but lim and limβˆ’ π‘₯β†’0

𝑓 (π‘₯)

π‘₯β†’0 𝑔(π‘₯)

1 = βˆ’βˆž. π‘₯

85. False, for example if 𝑓 (π‘₯) = 1βˆ•π‘₯, and 𝑔(π‘₯) = 1βˆ•π‘₯2 then lim

𝑓 (π‘₯)

π‘₯β†’0 𝑔(π‘₯)

= 0. does not exist, since lim+ π‘₯β†’0

1 =∞ π‘₯

= lim π‘₯ = 0 but the limits of 𝑓 (π‘₯) and 𝑔(π‘₯) do not exist, π‘₯β†’0

1 1 1 since lim+ = ∞ (and limβˆ’ = βˆ’βˆž) and lim 2 = ∞. π‘₯β†’0 π‘₯ π‘₯β†’0 π‘₯ π‘₯β†’0 π‘₯ 86. True, this follows from the multiplicative limit property: if lim π‘Ž(π‘₯) exists and lim 𝑏(π‘₯) exists then lim π‘Ž(π‘₯) β‹… 𝑏(π‘₯) exists (using π‘Ž(π‘₯) = 𝑓 (π‘₯)βˆ•π‘”(π‘₯) and 𝑏(π‘₯) = 𝑔(π‘₯)).

π‘₯β†’0

π‘₯β†’0

π‘₯β†’0

87. False, for example if 𝑔(π‘₯) = 1 when π‘₯ > 0 and 𝑔(π‘₯) = βˆ’1 when π‘₯ < 0, then setting 𝑓 (π‘₯) = 𝑔(π‘₯), 𝑓 (π‘₯) and using 𝑐 = 0 gives lim = lim 1 = 1. π‘₯β†’0 𝑔(π‘₯) π‘₯β†’0

Solutions for Section 1.10 EXERCISES 1. For each 𝛿 we determine whether the graph of 𝑓 (π‘₯) on the interval 3 βˆ’ 𝛿 < π‘₯ < 3 + 𝛿 stays in the shaded region 𝐿 βˆ’ πœ– < 𝑦 < 𝐿 + πœ– in the figure. Notice that as 𝛿 gets smaller, the interval gets shorter. (a) No for 𝛿 = 1. The graph of 𝑓 (π‘₯) on the interval 2 < π‘₯ < 4 extends outside the shaded region. (b) No for 𝛿 = 0.75. The graph of 𝑓 (π‘₯) on the interval 2.25 < π‘₯ < 3.75 extends outside the shaded region. (c) Yes for 𝛿 = 0.5. The graph of 𝑓 (π‘₯) on the interval 2.5 < π‘₯ < 3.5 fits inside the shaded region. (d) Yes for 𝛿 = 0.25. The graph of 𝑓 (π‘₯) on the interval 2.75 < π‘₯ < 3.25 fits inside the shaded region. (e) Yes for 𝛿 = 0.1. The graph of 𝑓 (π‘₯) on the interval 2.9 < π‘₯ < 3.1 fits inside the shaded region. 2. For each 𝛿 we determine whether the graph of 𝑔(π‘₯) on the interval 20 βˆ’ 𝛿 < π‘₯ < 20 + 𝛿 stays in the shaded region 𝐿 βˆ’ πœ– < 𝑦 < 𝐿 + πœ– in the figure. Notice that as 𝛿 gets smaller, the interval gets shorter. (a) No for 𝛿 = 0.5. The graph of 𝑔(π‘₯) on the interval 19.5 < π‘₯ < 20.5 extends outside the shaded region. (b) No for 𝛿 = 0.4. The graph of 𝑔π‘₯) on the interval 19.6 < π‘₯ < 20.4 extends outside the shaded region. (c) No for 𝛿 = 0.3. The graph of 𝑔(π‘₯) on the interval 19.7 < π‘₯ < 20.3 extends outside the shaded region. (d) Yes for 𝛿 = 0.2. The graph of 𝑔(π‘₯) on the interval 19.8 < π‘₯ < 20.2 fits inside the shaded region. (e) Yes for 𝛿 = 0.1. The graph of 𝑔(π‘₯) on the interval 19.9 < π‘₯ < 20.1 fits inside the shaded region. 3. By tracing on a calculator or solving equations, we find the following values of 𝛿: For πœ– = 0.2, 𝛿 ≀ 0.1. For πœ– = 0.1, 𝛿 ≀ 0.05. For πœ– = 0.02, 𝛿 ≀ 0.01. For πœ– = 0.01, 𝛿 ≀ 0.005. For πœ– = 0.002, 𝛿 ≀ 0.001. For πœ– = 0.001, 𝛿 ≀ 0.0005. 4. By tracing on a calculator or solving equations, we find the following values of 𝛿: For πœ– = 0.1, 𝛿 ≀ 0.46. For πœ– = 0.01, 𝛿 ≀ 0.21. For πœ– = 0.001, 𝛿 < 0.1. Thus, we can take 𝛿 ≀ 0.09. 5. Since |4π‘₯ βˆ’ 12| = 4|π‘₯ βˆ’ 3|, to get |4π‘₯ βˆ’ 12| < 0.1 we require that |π‘₯ βˆ’ 3| < 0.1βˆ•4 = 0.025. Thus we take 𝛿 = 0.025. 6. Since |(2π‘₯ βˆ’ 2) βˆ’ 0| = 2|π‘₯ βˆ’ 1|, to get |(2π‘₯ βˆ’ 2) βˆ’ 0| < 0.1 we require that |π‘₯ βˆ’ 1| < 0.1βˆ•2 = 0.05. Thus we take 𝛿 = 0.05. 7. Since |(5π‘₯ + 3) βˆ’ (βˆ’7)| = |5π‘₯ + 10| = 5|π‘₯ + 2|, to get |(5π‘₯ + 3) βˆ’ (βˆ’7)| < 0.1 we require that |π‘₯ + 2| < 0.1βˆ•5 = 0.02. Thus we take 𝛿 = 0.02. √ 8. Since |(π‘₯2 + 2) βˆ’ 2| = |π‘₯2 | = |π‘₯|2 , to get |(π‘₯2 + 2) βˆ’ 2| < 0.1 we require that |π‘₯| < 0.1 = 0.316. Thus we take 𝛿 = 0.316.


1.10 SOLUTIONS

121

PROBLEMS 9. The statement

lim 𝑔(β„Ž) = 𝐾

β„Žβ†’π‘Ž

means that we can make the value of 𝑔(β„Ž) as close to 𝐾 as we want by choosing β„Ž sufficiently close to, but not equal to, π‘Ž. In symbols, for any πœ– > 0, there is a 𝛿 > 0 such that |𝑔(β„Ž) βˆ’ 𝐾| < πœ–

for all 0 < |β„Ž βˆ’ π‘Ž| < 𝛿.

10. By tracing on a calculator or solving equations, we find the following values of 𝛿: For πœ– = 0.1, 𝛿 ≀ 0.1 For πœ– = 0.05, 𝛿 ≀ 0.05. For πœ– = 0.0007, 𝛿 ≀ 0.00007. 11. By tracing on a calculator or solving equations, we find the following values of 𝛿: For πœ– = 0.1, 𝛿 ≀ 0.45. For πœ– = 0.001, 𝛿 ≀ 0.0447. For πœ– = 0.00001, 𝛿 ≀ 0.00447. 12. We want to find 𝛿 > 0 such that if βˆ’π›Ώ < π‘₯ < 𝛿, then |𝑒π‘₯ βˆ’ 1| < 0.1. Observe that |𝑒π‘₯ βˆ’ 1| < 0.1 βˆ’0.1 < 𝑒π‘₯ βˆ’ 1 < 0.1 ln(0.9) < π‘₯ < ln(1.1), and that ln(0.9) = βˆ’0.105 and ln(1.1) = 0.095. We therefore choose 𝛿 = ln(1.1) so that βˆ’π›Ώ < π‘₯ < 𝛿 implies ln(0.9) < βˆ’ ln(1.1) < π‘₯ < ln(1.1), π‘₯

which, in turn, implies that |𝑒 βˆ’ 1| < 0.1 (see Figure 1.129). 𝑦 = 0.1

𝑦 = βˆ’0.1 π‘₯ = βˆ’ ln(1.1)

π‘₯ = ln(1.1) π‘₯

Figure 1.129: Graph of 𝑒 βˆ’ 1 with βˆ’ ln(1.1) < π‘₯ < ln(1.1) 13. We want to find 𝛿 > 0 such that if βˆ’π›Ώ < π‘₯ βˆ’ 1 < 𝛿, then | ln π‘₯| < 0.1. Observe that | ln π‘₯| < 0.1 βˆ’0.1 < ln π‘₯ < 0.1 π‘’βˆ’0.1 < π‘₯ < 𝑒0.1 βˆ’0.1

𝑒

βˆ’ 1 < π‘₯ βˆ’ 1 < 𝑒0.1 βˆ’ 1

and that 1 βˆ’ π‘’βˆ’0.1 = 0.095 and 𝑒0.1 βˆ’ 1 = 0.105. We therefore choose 𝛿 = 1 βˆ’ π‘’βˆ’0.1 so that βˆ’π›Ώ < π‘₯ βˆ’ 1 < 𝛿 implies π‘’βˆ’0.1 βˆ’ 1 < π‘₯ βˆ’ 1 < 1 βˆ’ π‘’βˆ’0.1 < 𝑒0.1 βˆ’ 1, which, in turn, implies that | ln π‘₯| < 0.1 (see Figure 1.130).


122

Chapter One /SOLUTIONS 𝑦 = 0.1

𝑦 = βˆ’0.1 π‘₯=1βˆ’π›Ώ

π‘₯=1+𝛿

Figure 1.130: Graph of ln π‘₯ with 1 βˆ’ 𝛿 < π‘₯ < 1 + 𝛿, where 𝛿 = 1 βˆ’ π‘’βˆ’0.1 . 14. We want to find 𝛿 > 0 such that if βˆ’π›Ώ < π‘₯ βˆ’ 1 < 𝛿, then | arctan π‘₯ βˆ’ (πœ‹βˆ•4)| < 0.1. Observe that | | |arctan π‘₯ βˆ’ πœ‹ | < 0.1 | 4 || | πœ‹ βˆ’0.1 < arctan π‘₯ βˆ’ < 0.1 4 πœ‹ πœ‹ βˆ’ 0.1 < arctan π‘₯ < + 0.1 4 4 ) ( ) ( πœ‹ πœ‹ βˆ’ 0.1 < π‘₯ < tan + 0.1 tan 4 4 ) ( ) ( πœ‹ πœ‹ βˆ’ 0.1 βˆ’ 1 < π‘₯ βˆ’ 1 < tan + 0.1 βˆ’ 1, tan 4 4 and that 1 βˆ’ tan((πœ‹βˆ•4) βˆ’ 0.1) = 0.182 and tan((πœ‹βˆ•4) + 0.1) βˆ’ 1 = 0.223. We therefore choose 𝛿 = 1 βˆ’ tan((πœ‹βˆ•4) βˆ’ 0.1) so that βˆ’π›Ώ < π‘₯ βˆ’ 1 < 𝛿 implies ) ( ) ( ) ( πœ‹ πœ‹ πœ‹ βˆ’ 0.1 βˆ’ 1 < π‘₯ βˆ’ 1 < 1 βˆ’ tan βˆ’ 0.1 < tan + 0.1 βˆ’ 1, tan 4 4 4 which, in turn, implies that | arctan π‘₯ βˆ’ (πœ‹βˆ•4)| < 0.1 (see Figure 1.131). 𝑦 = πœ‹4 + 0.1

𝑦 = πœ‹4 βˆ’ 0.1 π‘₯=1βˆ’π›Ώ

π‘₯=1+𝛿

Figure 1.131: Graph of arctan π‘₯ with 1 βˆ’ 𝛿 < π‘₯ < 1 + 𝛿, where 𝛿 = 1 βˆ’ tan((πœ‹βˆ•4) βˆ’ 0.01). 15. We want to find 𝛿 > 0 such that if βˆ’π›Ώ < π‘₯ βˆ’ 2 < 𝛿, then |(1βˆ•π‘₯) βˆ’ (1βˆ•2)| < 0.1. Observe that |1 1| | βˆ’ | < 0.1 |π‘₯ 2| | | 1 1 1 βˆ’ 0.1 < < + 0.1 2 π‘₯ 2 1 3 2 < < 5 π‘₯ 5 5 5 <π‘₯< 3 2 1 1 βˆ’ <π‘₯βˆ’2 < . 3 2


1.10 SOLUTIONS

123

We therefore choose 𝛿 = 1βˆ•3 so that βˆ’π›Ώ < π‘₯ βˆ’ 2 < 𝛿 implies 1 1 1 <π‘₯βˆ’2< < , 3 3 2 which, in turn, implies that |(1βˆ•π‘₯) βˆ’ (1βˆ•2)| < 0.1 (see Figure 1.132). βˆ’

𝑦 = 12 + 0.1

𝑦 = 12 βˆ’ 0.1 π‘₯ = 5βˆ•3

π‘₯ = 7βˆ•3

Figure 1.132: Graph of 1βˆ•π‘₯ with 5βˆ•3 < π‘₯ < 7βˆ•3. √ 16. We want to find 𝛿 > 0 such that if βˆ’π›Ώ < π‘₯ βˆ’ 4 < 𝛿, then | π‘₯ βˆ’ 2| < 0.1. Observe that √ | π‘₯ βˆ’ 2| < 0.1 √ 1.9 < π‘₯ < 2.1 3.61 < π‘₯ < 4.41 βˆ’0.39 < π‘₯ βˆ’ 4 < 0.41. We therefore choose 𝛿 = 0.39 so that βˆ’π›Ώ < π‘₯ βˆ’ 4 < 𝛿 implies βˆ’0.39 < π‘₯ βˆ’ 4 < 0.39 < 0.41, √ which, in turn, implies that | π‘₯ βˆ’ 2| < 0.1 (see Figure 1.133). 𝑦 = 2 + 0.1

𝑦 = 2 βˆ’ 0.1 π‘₯ = βˆ’0.39

π‘₯ = 0.39

√ Figure 1.133: Graph of π‘₯ with βˆ’0.39 < π‘₯ < 0.39.

17. From Table 1.17, it appears the limit is 0. This is confirmed by Figure 1.134. An appropriate window is βˆ’0.015 < π‘₯ < 0.015, βˆ’0.01 < 𝑦 < 0.01. 0.01

Table 1.17 π‘₯

𝑓 (π‘₯)

π‘₯

𝑓 (π‘₯)

0.1

0.0666

βˆ’0.0001

βˆ’0.0001

0.01

0.0067

βˆ’0.001

βˆ’0.0007

0.001

0.0007

βˆ’0.01

βˆ’0.0067

0.0001

0.0001

βˆ’0.1

βˆ’0.0666

βˆ’0.01 βˆ’0.015

Figure 1.134

0.015


124

Chapter One /SOLUTIONS

18. From Table 1.18, it appears the limit is 0. This is confirmed by Figure 1.135. An appropriate window is βˆ’0.0029 < π‘₯ < 0.0029, βˆ’0.01 < 𝑦 < 0.01. 0.01

Table 1.18 π‘₯

𝑓 (π‘₯)

π‘₯

𝑓 (π‘₯)

0.1

0.3365

βˆ’0.0001

βˆ’0.0004

0.01

0.0337

βˆ’0.001

βˆ’0.0034

0.001

0.0034

βˆ’0.01

βˆ’0.0337

0.0001

0.0004

βˆ’0.1

βˆ’0.3365

βˆ’0.01 βˆ’0.0029

0.0029

Figure 1.135

19. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯ βˆ’ 2| < 𝛿 with π‘₯ β‰  2, then |(5π‘₯ βˆ’ 6) βˆ’ 4| < πœ–. Observe that |(5π‘₯ βˆ’ 6) βˆ’ 4| = |5π‘₯ βˆ’ 10| = 5|π‘₯ βˆ’ 2|. Choose 𝛿 = πœ–βˆ•5. If |π‘₯ βˆ’ 2| < 𝛿 with π‘₯ β‰  2, we have |(5π‘₯ βˆ’ 6) βˆ’ 4| = 5|π‘₯ βˆ’ 2| < 5𝛿 = πœ–, proving that lim (5π‘₯ βˆ’ 6) = 4. π‘₯β†’2

20. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯ + 1| < 𝛿 with π‘₯ β‰  βˆ’1, then |(3π‘₯ + 1) + 2| < πœ–. Observe that |(3π‘₯ + 1) + 2| = |3π‘₯ + 3| = 3|π‘₯ + 1|. Choose 𝛿 = πœ–βˆ•3. If |π‘₯ + 1| < 𝛿 with π‘₯ β‰  βˆ’1, we have |(3π‘₯ + 1) + 2| = 3|π‘₯ + 1| < 3𝛿 = πœ–, proving that lim (3π‘₯ + 1) = βˆ’2. π‘₯β†’βˆ’1

21. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯| < 𝛿 with π‘₯ β‰  0, then |(βˆ’2π‘₯ + 3) βˆ’ 3| < πœ–. Observe that |(βˆ’2π‘₯ + 3) βˆ’ 3| = | βˆ’ 2π‘₯| = 2|π‘₯|. Choose 𝛿 = πœ–βˆ•2. If |π‘₯| < 𝛿 with π‘₯ β‰  0, we have |(βˆ’2π‘₯ + 3) βˆ’ 3| = 2|π‘₯| < 2𝛿 = πœ–, proving that lim (βˆ’2π‘₯ + 3) = 3. π‘₯β†’0

22. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯| < 𝛿 with π‘₯ β‰  0, then |(π‘₯2 + 2) βˆ’ 2| < πœ–. Observe that |(π‘₯2 + 2) βˆ’ 2| = |π‘₯2 | = |π‘₯|2 . Choose 𝛿 =

√

πœ–. If |π‘₯| < 𝛿 with π‘₯ β‰  0, we have |(π‘₯2 + 2) βˆ’ 2| = |π‘₯|2 < 𝛿 2 = πœ–,

proving that lim (π‘₯2 + 2) = 2. π‘₯β†’0

23. For any πœ– > 0, we want to find the 𝛿 such that | | | | |𝑔(π‘₯) βˆ’ 2| = |βˆ’π‘₯3 + 2 βˆ’ 2| = |π‘₯3 | < πœ–. | | | | Choose 𝛿 = πœ– 1βˆ•3 . Then if |π‘₯| < 𝛿 = πœ– 1βˆ•3 , it follows that |𝑔(π‘₯) βˆ’ 2| = ||π‘₯3 || < πœ–.


1.10 SOLUTIONS

125

24. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯ βˆ’ 1| < 𝛿 with π‘₯ β‰  βˆ’1, then | | 2π‘₯2 + π‘₯ βˆ’ 3 | βˆ’ 5|| < πœ–. | π‘₯βˆ’1 | | Observe that, if π‘₯ β‰  1, then | | (2π‘₯ + 3)(π‘₯ βˆ’ 1) | | 2π‘₯2 + π‘₯ βˆ’ 3 | βˆ’ 5|| = || βˆ’ 5|| = |2π‘₯ + 3 βˆ’ 5| = 2|π‘₯ βˆ’ 1|. | π‘₯βˆ’1 π‘₯ βˆ’ 1 | | | | Choose 𝛿 = πœ–βˆ•2. If |π‘₯ βˆ’ 1| < 𝛿 with π‘₯ β‰  1, we have | 2π‘₯2 + π‘₯ βˆ’ 3 | | βˆ’ 5|| = 2|π‘₯ βˆ’ 1| < 2𝛿 = πœ–, | π‘₯βˆ’1 | | 2π‘₯2 + π‘₯ βˆ’ 3 = 5. π‘₯βˆ’1 25. For any πœ– > 0, we must show that there exists 𝛿 > 0 such that, if |π‘₯ + 3| < 𝛿 with π‘₯ β‰  βˆ’3, then proving that lim π‘₯β†’1

| | π‘₯2 + 2π‘₯ βˆ’ 3 | + 4|| < πœ–. | π‘₯+3 | | Observe that, if π‘₯ β‰  βˆ’3, then | | (π‘₯ + 3)(π‘₯ βˆ’ 1) | | π‘₯2 + 2π‘₯ βˆ’ 3 | + 4|| = || + 4|| = |π‘₯ + 3|. | π‘₯+3 π‘₯ + 3 | | | | Choose 𝛿 = πœ–. If |π‘₯ + 3| < 𝛿 with π‘₯ β‰  βˆ’3, we have | | π‘₯2 + 2π‘₯ βˆ’ 3 | + 4|| = |π‘₯ + 3| < 𝛿 = πœ–, | π‘₯+3 | | π‘₯2 + 2π‘₯ βˆ’ 3 = βˆ’4. π‘₯+3 26. (a) We want to show that, no matter how close π‘₯ gets to 0, there will always be values of π‘₯ such that 𝑓 (π‘₯) is not close to 1. By choosing values of π‘₯ for which 𝑓 (π‘₯) = 0, we see that |𝑓 (π‘₯) βˆ’ 1| = 1; that is, the distance between 𝑓 (π‘₯) and 1 equals 1. For any nonzero integer 𝑛, we have proving that lim

π‘₯β†’βˆ’3

𝑓 (π‘₯) = 0 sin(1βˆ•π‘₯) = 0 1 = π‘›πœ‹ π‘₯ 1 , π‘₯= π‘›πœ‹ so 𝑓 (1βˆ•(π‘›πœ‹)) = 0. Choose πœ– to be any real number less than one, and consider any 𝛿 > 0. Then we can choose a positive integer 𝑛 large enough so that, if π‘₯ = 1βˆ•(π‘›πœ‹), then |π‘₯| < 𝛿. Thus, π‘₯ is close to 0, but 𝑓 (π‘₯) = 0 is not close to 1 because |𝑓 (π‘₯) βˆ’ 1| = 1 > πœ– (see Figure 1.136). This proves that lim 𝑓 (π‘₯) β‰  1. π‘₯β†’0

𝑦 1+πœ– 1 1βˆ’πœ– 1 π‘›πœ‹

𝛿

Figure 1.136

𝑓 (π‘₯) π‘₯


126

Chapter One /SOLUTIONS (b) We want to show that, no matter how close π‘₯ gets to 0, there will always be values of π‘₯ such that 𝑓 (π‘₯) is not close to 𝐿. By choosing values of π‘₯ for which 𝑓 (π‘₯) = 1, we see that |𝑓 (π‘₯) βˆ’ 𝐿| = |1 βˆ’ 𝐿|; that is, the distance between 𝑓 (π‘₯) and 𝐿 equals |1 βˆ’ 𝐿| > 0. Observe that 𝑓 (π‘₯) = 1 sin(1βˆ•π‘₯) = 1 πœ‹ 5πœ‹ 9πœ‹ 13πœ‹ 1 = , , , ,… π‘₯ 2 2 2 2 2 2 2 2 , , ,β‹―, π‘₯= , πœ‹ 5πœ‹ 9πœ‹ 13πœ‹ so 𝑓 (π‘₯) = 0 if π‘₯ = 2βˆ•((4𝑛 βˆ’ 3)πœ‹) for a positive integer 𝑛. Choose πœ– = |1 βˆ’ 𝐿|βˆ•2, and consider any 𝛿 > 0. Then we can choose a positive integer 𝑛 large enough so that, if π‘₯ = 2βˆ•((4𝑛 βˆ’ 3)πœ‹), then |π‘₯| < 𝛿. Thus, π‘₯ is close to 0, but 𝑓 (π‘₯) = 1 is not close to 𝐿 because |𝑓 (π‘₯) βˆ’ 𝐿| = |1 βˆ’ 𝐿| > πœ– (see Figure 1.137). This proves that lim 𝑓 (π‘₯) β‰  𝐿. π‘₯β†’0

𝑦 1

𝑓 (π‘₯)

𝐿+πœ–

2 (4π‘›βˆ’3)πœ‹

𝐿 𝛿

πΏβˆ’πœ–

π‘₯

Figure 1.137 27. (a) For any 𝑐, we have 𝑓 (𝑐) = π‘˜. This means |𝑓 (π‘₯) βˆ’ 𝑓 (𝑐)| = |π‘˜ βˆ’ π‘˜| = 0 for any π‘₯ and 𝑐. So given πœ– > 0, choose any 𝛿, for example 𝛿 = 1. Then |π‘₯ βˆ’ 𝑐| < 𝛿 implies |𝑓 (π‘₯) βˆ’ 𝑓 (𝑐)| = 0 < πœ–. So lim 𝑓 (π‘₯) = 𝑓 (𝑐), so 𝑓 is continuous π‘₯→𝑐 everywhere. (b) Given any πœ– > 0, we can take 𝛿 = πœ–, so that when |π‘₯ βˆ’ 𝑐| < 𝛿, |𝑔(π‘₯) βˆ’ 𝑔(𝑐)| = |π‘₯ βˆ’ 𝑐| < πœ–. So, lim 𝑔(π‘₯) = 𝑔(𝑐) and 𝑔 π‘₯→𝑐 is continuous everywhere. 28. The only change is that, instead of considering all π‘₯ near 𝑐, we only consider π‘₯ near to and greater than 𝑐. Thus the phrase β€œ|π‘₯ βˆ’ 𝑐| < 𝛿” must be replaced by β€œπ‘ < π‘₯ < 𝑐 + 𝛿.” Thus, we define lim 𝑓 (π‘₯) = 𝐿

π‘₯→𝑐 +

to mean that for any πœ– > 0 (as small as we want), there is a 𝛿 > 0 (sufficiently small) such that if 𝑐 < π‘₯ < 𝑐 + 𝛿, then |𝑓 (π‘₯) βˆ’ 𝐿| < πœ–. 29. The only change is that, instead of considering all π‘₯ near 𝑐, we only consider π‘₯ near to and less than 𝑐. Thus the phrase β€œ|π‘₯ βˆ’ 𝑐| < 𝛿” must be replaced by β€œπ‘ βˆ’ 𝛿 < π‘₯ < 𝑐.” Thus, we define lim 𝑓 (π‘₯) = 𝐿

π‘₯→𝑐 βˆ’

to mean that for any πœ– > 0 (as small as we want), there is a 𝛿 > 0 (sufficiently small) such that if 𝑐 βˆ’ 𝛿 < π‘₯ < 𝑐, then |𝑓 (π‘₯) βˆ’ 𝐿| < πœ–. 30. Instead of being β€œsufficiently close to 𝑐,” we want π‘₯ to be β€œsufficiently large.” Using 𝑁 to measure how large π‘₯ must be, we define lim 𝑓 (π‘₯) = 𝐿 π‘₯β†’βˆž

to mean that for any πœ– > 0 (as small as we want), there is a 𝑁 > 0 (sufficiently large) such that if π‘₯ > 𝑁, then |𝑓 (π‘₯)βˆ’πΏ| < πœ–. 31. (a) If 𝑏 = 0, then the property says limπ‘₯→𝑐 0 = 0, which is easy to see is true. πœ– , then multiplying by |𝑏| gives (b) If |𝑓 (π‘₯) βˆ’ 𝐿| < |𝑏| |𝑏||𝑓 (π‘₯) βˆ’ 𝐿| < πœ–. Since |𝑏||𝑓 (π‘₯) βˆ’ 𝐿| = |𝑏(𝑓 (π‘₯) βˆ’ 𝐿)| = |𝑏𝑓 (π‘₯) βˆ’ 𝑏𝐿|, we have |𝑏𝑓 (π‘₯) βˆ’ 𝑏𝐿| < πœ–.


1.10 SOLUTIONS

127

(c) Suppose that lim 𝑓 (π‘₯) = 𝐿. We want to show that lim 𝑏𝑓 (π‘₯) = 𝑏𝐿. If we are to have π‘₯→𝑐

π‘₯→𝑐

|𝑏𝑓 (π‘₯) βˆ’ 𝑏𝐿| < πœ–, then we will need |𝑓 (π‘₯) βˆ’ 𝐿| < We choose 𝛿 small enough that |π‘₯ βˆ’ 𝑐| < 𝛿

implies

πœ– . |𝑏|

|𝑓 (π‘₯) βˆ’ 𝐿| <

πœ– . |𝑏|

By part (b), this ensures that |𝑏𝑓 (π‘₯) βˆ’ 𝑏𝐿| < πœ–, as we wanted. 32. Suppose lim 𝑓 (π‘₯) = 𝐿1 and lim 𝑔(π‘₯) = 𝐿2 . Then we need to show that π‘₯→𝑐

π‘₯→𝑐

lim (𝑓 (π‘₯) + 𝑔(π‘₯)) = 𝐿1 + 𝐿2 . π‘₯→𝑐

Let πœ– > 0 be given. We need to show that we can choose 𝛿 > 0 so that whenever |π‘₯ βˆ’ 𝑐| < 𝛿, we will have |(𝑓 (π‘₯) + 𝑔(π‘₯)) βˆ’ (𝐿1 + 𝐿2 )| < πœ–. First choose 𝛿1 > 0 so that |π‘₯ βˆ’ 𝑐| < 𝛿1 implies |𝑓 (π‘₯) βˆ’ 𝐿1 | < πœ– ; we can do this since | | 2 lim 𝑓 (π‘₯) = 𝐿1 . Similarly, choose 𝛿2 > 0 so that |π‘₯ βˆ’ 𝑐| < 𝛿2 implies |𝑔(π‘₯) βˆ’ 𝐿2 | < 2πœ– . Now, set 𝛿 equal to the smaller of π‘₯→𝑐

𝛿1 and 𝛿2 . Thus |π‘₯ βˆ’ 𝑐| < 𝛿 will make both |π‘₯ βˆ’ 𝑐| < 𝛿1 and |π‘₯ βˆ’ 𝑐| < 𝛿2 . Then, for |π‘₯ βˆ’ 𝑐| < 𝛿, we have ) ( ) ( |𝑓 (π‘₯) + 𝑔(π‘₯) βˆ’ (𝐿1 + 𝐿2 )| = || 𝑓 (π‘₯) βˆ’ 𝐿1 + 𝑔(π‘₯) βˆ’ 𝐿2 || | | | | )| |( )| |( ≀ | 𝑓 (π‘₯) βˆ’ 𝐿1 | + | 𝑔(π‘₯) βˆ’ 𝐿2 | | | | | πœ– πœ– ≀ + = πœ–. 2 2 This proves limπ‘₯→𝑐 (𝑓 (π‘₯) + 𝑔(π‘₯)) = limπ‘₯→𝑐 𝑓 (π‘₯) + limπ‘₯→𝑐 𝑔(π‘₯), which is the result we wanted to prove.

33. (a) We need to show that for any given πœ– > 0, there is a 𝛿 > 0 so that √ |π‘₯ βˆ’ 𝑐| < 𝛿 implies |𝑓 (π‘₯)𝑔(π‘₯)| < πœ–. If πœ– > 0 is given, choose 𝛿1 so that when |π‘₯ βˆ’ 𝑐| < 𝛿1 , we have |𝑓 (π‘₯)| < πœ–. This can be done since limπ‘₯β†’0 𝑓 (π‘₯) = 0. √ Similarly, choose 𝛿2 so that when |π‘₯ βˆ’ 𝑐| < 𝛿2 , we have |𝑔(π‘₯)| < πœ–. Then, if we take 𝛿 to be the smaller of 𝛿1 √ √ and 𝛿2 , we’ll have that |π‘₯ βˆ’ 𝑐| < 𝛿 implies both |𝑓 (π‘₯)| < πœ– and |𝑔(π‘₯)| < πœ–. So when |π‘₯ βˆ’ 𝑐| < 𝛿, we have √ √ |𝑓 (π‘₯)𝑔(π‘₯)| = |𝑓 (π‘₯)| |𝑔(π‘₯)| < πœ– β‹… πœ– = πœ–. Thus lim 𝑓 (π‘₯)𝑔(π‘₯) = 0. π‘₯→𝑐 ( )( ) (b) 𝑓 (π‘₯) βˆ’ 𝐿1 𝑔(π‘₯) βˆ’ 𝐿2 + 𝐿1 𝑔(π‘₯) + 𝐿2 𝑓 (π‘₯) βˆ’ 𝐿1 𝐿2 = 𝑓((π‘₯)𝑔(π‘₯) βˆ’ 𝐿)1 𝑔(π‘₯) βˆ’ 𝐿2 𝑓 (π‘₯) + 𝐿1 𝐿2 + 𝐿1 𝑔(π‘₯) + 𝐿2 𝑓 (π‘₯) βˆ’ 𝐿1 𝐿2 = 𝑓 (π‘₯)𝑔(π‘₯). ( ) (c) lim 𝑓 (π‘₯) βˆ’ 𝐿1 = lim 𝑓 (π‘₯) βˆ’ lim 𝐿1 = 𝐿1 βˆ’ 𝐿1 = 0, using the second limit property. Similarly, lim 𝑔(π‘₯) βˆ’ 𝐿2 = 0. π‘₯→𝑐 π‘₯→𝑐 π‘₯→𝑐 π‘₯→𝑐 ( ) ( ) ( )( ) (d) Since lim 𝑓 (π‘₯) βˆ’ 𝐿1 = lim 𝑔(π‘₯) βˆ’ 𝐿2 = 0, we have that lim 𝑓 (π‘₯) βˆ’ 𝐿1 𝑔(π‘₯) βˆ’ 𝐿2 = 0 by part (a). π‘₯→𝑐 π‘₯→𝑐 π‘₯→𝑐 (e) From part (b), we have (( )( ) ) 𝑓 (π‘₯) βˆ’ 𝐿1 𝑔(π‘₯) βˆ’ 𝐿2 + 𝐿1 𝑔(π‘₯) + 𝐿2 𝑓 (π‘₯) βˆ’ 𝐿1 𝐿2 ( )( ) = lim 𝑓 (π‘₯) βˆ’ 𝐿1 𝑔(π‘₯) βˆ’ 𝐿2 + lim 𝐿1 𝑔(π‘₯) + lim 𝐿2 𝑓 (π‘₯) + lim(βˆ’πΏ1 𝐿2 )

lim 𝑓 (π‘₯)𝑔(π‘₯) = lim π‘₯→𝑐

π‘₯→𝑐 π‘₯→𝑐

π‘₯→𝑐

(using limit property 2) = 0 + 𝐿1 lim 𝑔(π‘₯) + 𝐿2 lim 𝑓 (π‘₯) βˆ’ 𝐿1 𝐿2 π‘₯→𝑐

π‘₯→𝑐

(using limit property 1 and part (d)) = 𝐿1 𝐿2 + 𝐿2 𝐿1 βˆ’ 𝐿1 𝐿2 = 𝐿1 𝐿2 .

Strengthen Your Understanding 34. False. For example, define 𝑓 as follows: 𝑓 (π‘₯) =

{

2π‘₯ + 1 if π‘₯ β‰  2.99 1000 if π‘₯ = 2.99.

Then 𝑓 (2.9) = 2(2.9) + 1 = 6.8, whereas 𝑓 (2.99) = 1000.

π‘₯→𝑐

π‘₯→𝑐


128

Chapter One /SOLUTIONS

35. False. For example, define 𝑓 as follows: 𝑓 (π‘₯) =

{

2π‘₯ + 1 βˆ’1000

if π‘₯ β‰  3.01 if π‘₯ = 3.01.

Then 𝑓 (3.1) = 2(3.1) + 1 = 7.2, whereas 𝑓 (3.01) = βˆ’1000. 36. False. For some functions we need to pick smaller values of 𝛿. For example, if 𝑓 (π‘₯) = π‘₯1βˆ•3 + 2 and 𝑐 = 0 and 𝐿 = 2, then 𝑓 (π‘₯) is within 10βˆ’3 of 2 if |π‘₯1βˆ•3 | < 10βˆ’3 . This only happens if π‘₯ is within (10βˆ’3 )3 = 10βˆ’9 of 0. If π‘₯ = 10βˆ’3 then π‘₯1βˆ•3 = (10βˆ’3 )1βˆ•3 = 10βˆ’1 , which is too large. 37. False. The definition of a limit guarantees that, for any positive πœ–, there is a 𝛿. This statement, which guarantees an πœ– for a specific 𝛿 = 10βˆ’3 , is not equivalent to limπ‘₯→𝑐 𝑓 (π‘₯) = 𝐿. For example, consider a function with a vertical asymptote within 10βˆ’3 of 0, such as 𝑐 = 0, 𝐿 = 0, 𝑓 (π‘₯) = π‘₯βˆ•(π‘₯ βˆ’ 10βˆ’4 ). 38. True. This is equivalent to the definition of a limit. 39. False. Although π‘₯ may be far from 𝑐, the value of 𝑓 (π‘₯) could be close to 𝐿. For example, suppose 𝑓 (π‘₯) = 𝐿, the constant function. 40. False. The definition of the limit says that if π‘₯ is within 𝛿 of 𝑐, then 𝑓 (π‘₯) is within πœ– of 𝐿, not the other way round.

Solutions for Chapter 1 Review EXERCISES 1. The line of slope π‘š through the point (π‘₯0 , 𝑦0 ) has equation 𝑦 βˆ’ 𝑦0 = π‘š(π‘₯ βˆ’ π‘₯0 ), so the line we want is 𝑦 βˆ’ 0 = 2(π‘₯ βˆ’ 5) 𝑦 = 2π‘₯ βˆ’ 10. 2. We want a function of the form 𝑦 = π‘Ž(π‘₯ βˆ’ β„Ž)2 + π‘˜, with π‘Ž < 0 because the parabola opens downward. Since (β„Ž, π‘˜) is the vertex, we must take β„Ž = 2, π‘˜ = 5, but we can take any negative value of π‘Ž. Figure 1.138 shows the graph with π‘Ž = βˆ’1, namely 𝑦 = βˆ’(π‘₯ βˆ’ 2)2 + 5. 𝑦

(2, 5)

π‘₯

Figure 1.138: Graph of 𝑦 = βˆ’(π‘₯ βˆ’ 2)2 + 5 3. A parabola with π‘₯-intercepts Β±1 has an equation of the form 𝑦 = π‘˜(π‘₯ βˆ’ 1)(π‘₯ + 1). Substituting the point π‘₯ = 0, 𝑦 = 3 gives

3 = π‘˜(βˆ’1)(1)

so

π‘˜ = βˆ’3.

Thus, the equation we want is 𝑦 = βˆ’3(π‘₯ βˆ’ 1)(π‘₯ + 1) 𝑦 = βˆ’3π‘₯2 + 3.


SOLUTIONS to Review Problems for Chapter One 4. The equation of the whole circle is

129

√ π‘₯2 + 𝑦2 = ( 2)2 , √ 𝑦 = βˆ’ 2 βˆ’ π‘₯2 .

so the bottom half is

5. A circle with center (β„Ž, π‘˜) and radius π‘Ÿ has equation (π‘₯ βˆ’ β„Ž)2 + (𝑦 βˆ’ π‘˜)2 = π‘Ÿ2 . Thus β„Ž = βˆ’1, π‘˜ = 2, and π‘Ÿ = 3, giving (π‘₯ + 1)2 + (𝑦 βˆ’ 2)2 = 9. Solving for 𝑦, and taking the positive square root gives the top half, so (𝑦 βˆ’ 2)2 = 9 βˆ’ (π‘₯ + 1)2 √ 𝑦 = 2 + 9 βˆ’ (π‘₯ + 1)2 . See Figure 1.139. 𝑦

3 -

(βˆ’1, 2)

π‘₯

√ Figure 1.139: Graph of 𝑦 = 2 + 9 βˆ’ (π‘₯ + 1)2 6. A cubic polynomial of the form 𝑦 = π‘Ž(π‘₯ βˆ’ 1)(π‘₯ βˆ’ 5)(π‘₯ βˆ’ 7) has the correct intercepts for any value of π‘Ž β‰  0. Figure 1.140 shows the graph with π‘Ž = 1, namely 𝑦 = (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 5)(π‘₯ βˆ’ 7). 𝑦

1

5

7

π‘₯

Figure 1.140: Graph of 𝑦 = (π‘₯ βˆ’ 1)(π‘₯ βˆ’ 5)(π‘₯ βˆ’ 7) 7. Since the vertical asymptote is π‘₯ = 2, we have 𝑏 = βˆ’2. The fact that the horizontal asymptote is 𝑦 = βˆ’5 gives π‘Ž = βˆ’5. So βˆ’5π‘₯ . π‘₯βˆ’2 8. The amplitude of this function is 5, and its period is 2πœ‹, so 𝑦 = 5 cos π‘₯. 𝑦=

9. See Figure 1.141. heart rate

time

administration of drug

Figure 1.141


130

Chapter One /SOLUTIONS

10. Factoring gives

(2 βˆ’ π‘₯)(2 + π‘₯) . π‘₯(π‘₯ + 1) The values of π‘₯ which make 𝑔(π‘₯) undefined are π‘₯ = 0 and π‘₯ = βˆ’1, when the denominator is 0. So the domain is all π‘₯ β‰  0, βˆ’1. Solving 𝑔(π‘₯) = 0 means one of the numerator’s factors is 0, so π‘₯ = Β±2. 𝑔(π‘₯) =

11. (a) The domain of 𝑓 is the set of values of π‘₯ for which the function is defined. Since the function is defined by the graph and the graph goes from π‘₯ = 0 to π‘₯ = 7, the domain of 𝑓 is [0, 7]. (b) The range of 𝑓 is the set of values of 𝑦 attainable over the domain. Looking at the graph, we can see that 𝑦 gets as high as 5 and as low as βˆ’2, so the range is [βˆ’2, 5]. (c) Only at π‘₯ = 5 does 𝑓 (π‘₯) = 0. So 5 is the only zero of 𝑓 (π‘₯). (d) Looking at the graph, we can see that 𝑓 (π‘₯) is decreasing on (1, 7). (e) The graph indicates that 𝑓 (π‘₯) is concave up at π‘₯ = 6. (f) The value 𝑓 (4) is the 𝑦-value that corresponds to π‘₯ = 4. From the graph, we can see that 𝑓 (4) is approximately 1. (g) This function is not invertible, since it fails the horizontal-line test. A horizontal line at 𝑦 = 3 would cut the graph of 𝑓 (π‘₯) in two places, instead of the required one. 12. (a) 𝑓 (𝑛) + 𝑔(𝑛) = (3𝑛2 βˆ’ 2) + (𝑛 + 1) = 3𝑛2 + 𝑛 βˆ’ 1. (b) 𝑓 (𝑛)𝑔(𝑛) = (3𝑛2 βˆ’ 2)(𝑛 + 1) = 3𝑛3 + 3𝑛2 βˆ’ 2𝑛 βˆ’ 2. (c) The domain of 𝑓 (𝑛)βˆ•π‘”(𝑛) is defined everywhere where 𝑔(𝑛) β‰  0, i.e. for all 𝑛 β‰  βˆ’1. (d) 𝑓 (𝑔(𝑛)) = 3(𝑛 + 1)2 βˆ’ 2 = 3𝑛2 + 6𝑛 + 1. (e) 𝑔(𝑓 (𝑛)) = (3𝑛2 βˆ’ 2) + 1 = 3𝑛2 βˆ’ 1. 13. (a) Since π‘š = 𝑓 (𝐴), we see that 𝑓 (100) represents the value of π‘š when 𝐴 = 100. Thus 𝑓 (100) is the minimum annual gross income needed (in thousands) to take out a 30-year mortgage loan of $100,000 at an interest rate of 6%. (b) Since π‘š = 𝑓 (𝐴), we have 𝐴 = 𝑓 βˆ’1 (π‘š). We see that 𝑓 βˆ’1 (75) represents the value of 𝐴 when π‘š = 75, or the size of a mortgage loan that could be obtained on an income of $75,000. log 7 = 1.209. 14. Taking logs of both sides yields 𝑑 log 5 = log 7, so 𝑑 = log 5 log 2 β‰ˆ 35.003. 15. 𝑑 = log 1.02 ( )𝑑 16. Collecting similar factors yields 32 = 57 , so ( ) log 57 𝑑= ( ) = βˆ’0.830. log 32 17. Collecting similar factors yields

(

1.04 1.03

)𝑑

= 12.01 . Solving for 𝑑 yields 5.02 ) ( log 12.01 5.02 𝑑= ( ) = 90.283. log 1.04 1.03

18. We want 2𝑑 = π‘’π‘˜π‘‘ so 2 = π‘’π‘˜ and π‘˜ = ln 2 = 0.693. Thus 𝑃 = 𝑃0 𝑒0.693𝑑 . 19. We want 0.2𝑑 = π‘’π‘˜π‘‘ so 0.2 = π‘’π‘˜ and π‘˜ = ln 0.2 = βˆ’1.6094. Thus 𝑃 = 5.23π‘’βˆ’1.6094𝑑 . 20. 𝑓 (π‘₯) = ln π‘₯, 3

21. 𝑓 (π‘₯) = π‘₯ ,

𝑔(π‘₯) = π‘₯3 . (Another possibility: 𝑓 (π‘₯) = 3π‘₯,

𝑔(π‘₯) = ln π‘₯.)

𝑔(π‘₯) = ln π‘₯.

22. The amplitude is 5. The period is 6πœ‹. See Figure 1.142. 𝑦 5

βˆ’6πœ‹ βˆ’ 9πœ‹ βˆ’3πœ‹ βˆ’ 3πœ‹ 2

2

3πœ‹ 2

3πœ‹

βˆ’5

Figure 1.142

9πœ‹ 2

π‘₯

( ) 6πœ‹ 𝑦 = 5 sin 13 π‘₯


SOLUTIONS to Review Problems for Chapter One

131

23. The amplitude is 2. The period is 2πœ‹βˆ•5. See Figure 1.143. 𝑦 6 4 2 βˆ’ 4πœ‹ 5

𝑦 = 4 βˆ’ 2 cos(5π‘₯)

βˆ’ 2πœ‹ 5

2πœ‹ 5

4πœ‹ 5

π‘₯

Figure 1.143

24. (a) We determine the amplitude of 𝑦 by looking at the coefficient of the cosine term. Here, the coefficient is 1, so the amplitude of 𝑦 is 1. Note that the constant term does not affect the amplitude. (b) We know that the cosine function cos π‘₯ repeats itself at π‘₯ = 2πœ‹, so the function cos(3π‘₯) must repeat itself when 3π‘₯ = 2πœ‹, or at π‘₯ = 2πœ‹βˆ•3. So the period of 𝑦 is 2πœ‹βˆ•3. Here as well the constant term has no effect. (c) The graph of 𝑦 is shown in the figure below. 𝑦 6 5 4

2πœ‹ 3

π‘₯

25. (a) Since 𝑓 (π‘₯) is an odd polynomial with a positive leading coefficient, it follows that 𝑓 (π‘₯) β†’ ∞ as π‘₯ β†’ ∞ and 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ βˆ’βˆž. (b) Since 𝑓 (π‘₯) is an even polynomial with negative leading coefficient, it follows that 𝑓 (π‘₯) β†’ βˆ’βˆž as π‘₯ β†’ ±∞. (c) As π‘₯ β†’ ±∞, π‘₯4 β†’ ∞, so π‘₯βˆ’4 = 1βˆ•π‘₯4 β†’ 0. (d) As π‘₯ β†’ ±∞, the lower-degree terms of 𝑓 (π‘₯) become insignificant, and 𝑓 (π‘₯) becomes approximated by the highest degree terms in its numerator and denominator. So as π‘₯ β†’ ±∞, 𝑓 (π‘₯) β†’ 6. 26. Exponential growth dominates power growth as π‘₯ β†’ ∞, so 10 β‹… 2π‘₯ is larger. 27. As π‘₯ β†’ ∞, 0.25π‘₯1βˆ•2 is larger than 25,000π‘₯βˆ’3 . 28. This is a line with slope βˆ’3βˆ•7 and 𝑦-intercept 3, so a possible formula is 3 𝑦 = βˆ’ π‘₯ + 3. 7 29. Starting with the general exponential equation 𝑦 = π΄π‘’π‘˜π‘₯ , we first find that for (0, 1) to be on the graph, we must have 𝐴 = 1. Then to make (3, 4) lie on the graph, we require 4 = 𝑒3π‘˜ ln 4 = 3π‘˜ ln 4 β‰ˆ 0.4621. π‘˜= 3 Thus the equation is

𝑦 = 𝑒0.4621π‘₯ .

Alternatively, we can use the form 𝑦 = π‘Žπ‘₯ , in which case we find 𝑦 = (1.5874)π‘₯ .


132

Chapter One /SOLUTIONS

30. This looks like an exponential function. The 𝑦-intercept is 3 and we use the form 𝑦 = 3π‘’π‘˜π‘‘ . We substitute the point (5, 9) to solve for π‘˜: 9 = 3π‘’π‘˜5 3 = 𝑒5π‘˜ ln 3 = 5π‘˜ π‘˜ = 0.2197. A possible formula is

𝑦 = 3𝑒0.2197𝑑 .

Alternatively, we can use the form 𝑦 = 3π‘Žπ‘‘ , in which case we find 𝑦 = 3(1.2457)𝑑 . 31. 𝑦 = βˆ’π‘˜π‘₯(π‘₯ + 5) = βˆ’π‘˜(π‘₯2 + 5π‘₯), where π‘˜ > 0 is any constant. 32. Since this function has a 𝑦-intercept at (0, 2), we expect it to have the form 𝑦 = 2π‘’π‘˜π‘₯ . Again, we find π‘˜ by forcing the other point to lie on the graph: 1 = 2𝑒2π‘˜ 1 = 𝑒2π‘˜ 2 ( ) 1 = 2π‘˜ ln 2 ln( 21 ) π‘˜= β‰ˆ βˆ’0.34657. 2 This value is negative, which makes sense since the graph shows exponential decay. The final equation, then, is 𝑦 = 2π‘’βˆ’0.34657π‘₯ . Alternatively, we can use the form 𝑦 = 2π‘Žπ‘₯ , in which case we find 𝑦 = 2(0.707)π‘₯ . 33. 𝑧 = 1 βˆ’ cos πœƒ 34. 𝑦 = π‘˜(π‘₯ + 2)(π‘₯ + 1)(π‘₯ βˆ’ 1) = π‘˜(π‘₯3 + 2π‘₯2 βˆ’ π‘₯ βˆ’ 2), where π‘˜ > 0 is any constant. 35. π‘₯ = π‘˜π‘¦(𝑦 βˆ’ 4) = π‘˜(𝑦2 βˆ’ 4𝑦), where π‘˜ > 0 is any constant. ( ) πœ‹π‘‘ 36. 𝑦 = 5 sin 20 37. This looks like a fourth degree polynomial with roots at βˆ’5 and βˆ’1 and a double root at 3. The leading coefficient is negative, and so a possible formula is 𝑦 = βˆ’(π‘₯ + 5)(π‘₯ + 1)(π‘₯ βˆ’ 3)2 . 38. This looks like a rational function. There are vertical asymptotes at π‘₯ = βˆ’2 and π‘₯ = 2 and so one possibility for the denominator is π‘₯2 βˆ’ 4. There is a horizontal asymptote at 𝑦 = 3 and so the numerator might be 3π‘₯2 . In addition, 𝑦(0) = 0 which is the case with the numerator of 3π‘₯2 . A possible formula is 𝑦=

3π‘₯2 π‘₯2 βˆ’ 4

.

39. There are many solutions for a graph like this one. The simplest is 𝑦 = 1 βˆ’ π‘’βˆ’π‘₯ , which gives the graph of 𝑦 = 𝑒π‘₯ , flipped over the π‘₯-axis and moved up by 1. The resulting graph passes through the origin and approaches 𝑦 = 1 as an upper bound, the two features of the given graph. 40. The graph is a sine curve which has been shifted up by 2, so 𝑓 (π‘₯) = (sin π‘₯) + 2. 41. This graph has period 5, amplitude 1 and no vertical shift or horizontal shift from sin π‘₯, so it is given by ) ( 2πœ‹ π‘₯ . 𝑓 (π‘₯) = sin 5 42. Since the denominator, π‘₯2 + 1, is continuous and never zero, 𝑔(π‘₯) is continuous on [βˆ’1, 1].


SOLUTIONS to Review Problems for Chapter One

133

43. Since

1 1 = , (1 βˆ’ π‘₯)(1 + π‘₯) 1 βˆ’ π‘₯2 we see that β„Ž(π‘₯) is not defined at π‘₯ = βˆ’1 or at π‘₯ = 1, so β„Ž(π‘₯) is not continuous on [βˆ’1, 1]. β„Ž(π‘₯) =

44. (a) lim 𝑓 (π‘₯) = 1. π‘₯β†’0

(b) lim 𝑓 (π‘₯) does not exist. π‘₯β†’1

(c) lim 𝑓 (π‘₯) = 1. π‘₯β†’2

(d) limβˆ’ 𝑓 (π‘₯) = 0. π‘₯β†’3

⎧ π‘₯3 (2π‘₯ βˆ’ 6) 3 π‘₯>3 π‘₯3 |2π‘₯ βˆ’ 6| βŽͺ π‘₯ βˆ’ 3 = 2π‘₯ , 45. 𝑓 (π‘₯) = =⎨ 3 π‘₯ (βˆ’2π‘₯ + 6) π‘₯βˆ’3 βŽͺ = βˆ’2π‘₯3 , π‘₯ < 3 ⎩ π‘₯βˆ’3 Figure 1.144 confirms that lim+ 𝑓 (π‘₯) = 54 while limβˆ’ 𝑓 (π‘₯) = βˆ’54; thus lim 𝑓 (π‘₯) does not exist. π‘₯β†’3

π‘₯β†’3

π‘₯β†’3

100

𝑓 (π‘₯)

50 0

1

2 3

4

π‘₯

βˆ’50 βˆ’100

Figure 1.144 ⎧ 𝑒π‘₯ βˆ’1 < π‘₯ < 0 βŽͺ 46. 𝑓 (π‘₯) = ⎨ 1 π‘₯=0 βŽͺ 0<π‘₯<1 ⎩ cos π‘₯ Figure 1.145 confirms that limβˆ’ 𝑓 (π‘₯) = limβˆ’ 𝑒π‘₯ = 𝑒0 = 1, and that lim 𝑓 (π‘₯) = lim cos π‘₯ = cos 0 = 1, so lim 𝑓 (π‘₯) = 1.

π‘₯β†’0

π‘₯β†’0

π‘₯β†’0+

π‘₯β†’0+

π‘₯β†’0

1 𝑓 (π‘₯)

βˆ’1

0

1

π‘₯

Figure 1.145 47. (a) As 𝑑 approaches βˆ’2 from either side, the values of 𝑔(𝑑) get closer and closer to βˆ’5, so the limit appears to be about βˆ’5. (b) As 𝑑 approaches 0 from either side, the values of 𝑔(𝑑) get closer and closer to βˆ’1, so the limit appears to be about βˆ’1. (c) As 𝑑 approaches 1, the values of 𝑔(𝑑) get closer and closer to 4 on one side of 𝑑 = 1 and get closer and closer to a value less than 1 on the other side of 𝑑 = 1. Thus the limit does not exist. (d) As 𝑑 approaches 3 from either side, the values of 𝑔(𝑑) become arbitrarily large, so the limit does not exist. 48. (a) As π‘₯ approaches βˆ’2 from either side, the values of 𝑓 (π‘₯) get closer and closer to 3, so the limit appears to be about 3. (b) As π‘₯ approaches 0 from either side, the values of 𝑓 (π‘₯) get closer and closer to 7. (Recall that to find a limit, we are interested in what happens to the function near π‘₯ but not at π‘₯.) The limit appears to be about 7. (c) As π‘₯ approaches 2 from either side, the values of 𝑓 (π‘₯) get closer and closer to 3 on one side of π‘₯ = 2 and get closer and closer to 2 on the other side of π‘₯ = 2. Thus the limit does not exist. (d) As π‘₯ approaches 4 from either side, the values of 𝑓 (π‘₯) get closer and closer to 8. (Again, recall that we don’t care what happens right at π‘₯ = 4.) The limit appears to be about 8.


134

Chapter One /SOLUTIONS

49. Yes, because the denominator is never zero. 50. Yes, because 2π‘₯ + π‘₯2βˆ•3 is defined for all π‘₯. 51. No, because sin 0 = 0. 52. No, because 𝑒π‘₯ βˆ’ 1 = 0 at π‘₯ = 0. 53. For βˆ’1 ≀ πœƒ ≀ 1, βˆ’1 ≀ 𝑦 ≀ 1, the graph of 𝑦 =

cos πœƒ βˆ’ 1 is shown in Figure 1.146. The graph suggests that πœƒ cos πœƒ βˆ’ 1 = 0. lim πœƒβ†’0 πœƒ 𝑦

1 𝑦 = cosπœƒπœƒβˆ’1

βˆ’1

πœƒ

1

βˆ’1

Figure 1.146 54. For βˆ’0.5 ≀ πœƒ ≀ 0.5, 0 ≀ 𝑦 ≀ 0.5, the graph of 𝑦 = curve, we see that lim

πœƒ

πœƒβ†’0 tan(3πœƒ)

πœƒ is shown in Figure 1.147. Therefore, by tracing along the tan(3πœƒ)

= 0.3333 …. 𝑦 0.5

βˆ’0.5

πœƒ 𝑦 = tan(3πœƒ)

0

0.5

πœƒ

Figure 1.147 3β„Ž βˆ’ 1 in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and 0 ≀ 𝑦 ≀ 1.5 appears to indicate 𝑦 β†’ 1.1 as β„Ž β†’ 0. By 55. A graph of 𝑦 = β„Ž zooming in on the graph, we can estimate the limit more accurately. Therefore, we estimate that 3β„Ž βˆ’ 1 = 1.098. β„Žβ†’0 β„Ž lim

sin(3β„Ž) in a window such as βˆ’0.5 ≀ β„Ž ≀ 0.5 and 0 ≀ 𝑦 ≀ 4 appears to indicate 𝑦 β†’ 3 as β„Ž β†’ 0. 56. A graph of 𝑦 = β„Ž Therefore, we estimate that sin(3β„Ž) = 3. lim β„Žβ†’0 β„Ž 57. (a) Substituting π‘₯-values into 𝑓 (π‘₯) gives: π‘₯

0.9

0.99

1.01

1.1

𝑓 (π‘₯)

1.054

1.005

0.995

0.953

(b) Since the values of 𝑓 (π‘₯) appear to get closer and closer to 1 as π‘₯ gets closer and closer to 1, we estimate lim

ln π‘₯

π‘₯β†’1 π‘₯ βˆ’ 1

Notice that 𝑓 (π‘₯) =

ln π‘₯ is undefined at π‘₯ = 1. π‘₯βˆ’1

= 1.


SOLUTIONS to Review Problems for Chapter One

135

58. (a) Substituting π‘₯-values into 𝑓 (π‘₯) gives: π‘₯

0.9

0.99

1.01

1.1

𝑓 (π‘₯)

1.949

1.995

2.005

2.049

(b) Since the values of 𝑓 (π‘₯) appear to get closer and closer to 2 as π‘₯ gets closer and closer to 1, we estimate π‘₯βˆ’1 = 2. lim √ π‘₯β†’1 π‘₯βˆ’1 π‘₯βˆ’1 is undefined at π‘₯ = 1. Notice that 𝑓 (π‘₯) = √ π‘₯βˆ’1 59. Since the value of π‘₯2 increases faster than the value of ln π‘₯, we know that lim

π‘₯β†’βˆž

ln π‘₯ approaches zero as π‘₯ β†’ ∞. π‘₯2

ln π‘₯ = 0. π‘₯2 60. Since the value of 𝑒π‘₯ βˆ’ 2 grows arbitrarily large as π‘₯ β†’ ∞ while the numerator remains constant, the value of the function approaches zero. 2 = 0. Thus, lim π‘₯ π‘₯β†’βˆž 𝑒 βˆ’ 2 61. For large values of π‘₯, βˆ’5π‘₯2 + 2 behaves like βˆ’5π‘₯2 and 3π‘₯2 behaves like 3π‘₯2 , so (βˆ’5π‘₯2 + 2)βˆ•(3π‘₯2 ) behaves like βˆ’5π‘₯2 βˆ•3π‘₯2 . Thus 5 βˆ’5π‘₯2 + 2 βˆ’5π‘₯2 lim = lim =βˆ’ . 2 π‘₯β†’βˆž π‘₯β†’βˆž 3π‘₯2 3 3π‘₯ Thus, lim

π‘₯β†’βˆž

though answers will vary. 62. Possible answers are 𝑓 (π‘₯) = π‘₯ + 4 and 𝑓 (π‘₯) = 5π‘₯βˆ’5 π‘₯βˆ’1 2

63. Possible answers are 𝑓 (π‘₯) = 12 + π‘₯1 and 𝑓 (π‘₯) = 2π‘₯π‘₯2 +3 though answers will vary. 64. (a) When π‘₯ < 2, 𝑔(π‘₯) = π‘₯2 βˆ’ π‘₯. So as π‘₯ approaches 2 from the left, 𝑔(π‘₯) approaches 22 βˆ’ 2 = 2. So lim 𝑔(π‘₯) = 2.

π‘₯β†’2βˆ’

(b) When π‘₯ > 2, 𝑔(π‘₯) = 4βˆ•π‘₯. So as π‘₯ approaches 2 from the right, 𝑔(π‘₯) approaches 4βˆ•2 = 2. So lim 𝑔(π‘₯) = 2.

π‘₯β†’2+

(c) As π‘₯ approaches 2 from either side, 𝑔(π‘₯) approaches 2. Therefore, lim 𝑔(π‘₯) = 2. π‘₯β†’2

(d) For π‘₯ > 2, 𝑔(π‘₯) = 4βˆ•π‘₯. As π‘₯ approaches 3 from the left, π‘₯ is greater than 2, so 𝑔(π‘₯) approaches 4βˆ•3. Thus lim 𝑔(π‘₯) =

π‘₯β†’3βˆ’

4 . 3

65. (a) For π‘₯ < 2, we have 𝑓 (π‘₯) = 3π‘₯ βˆ’ 5, so as π‘₯ approaches 2 from the left, we have lim 𝑓 (π‘₯) = 3(2) βˆ’ 5 = 1.

π‘₯β†’2βˆ’

(b) For π‘₯ > 2, we have 𝑓 (π‘₯) = 3 βˆ’ 2π‘₯, so as π‘₯ approaches 2 from the right, we have lim 𝑓 (π‘₯) = 3 βˆ’ 2(2) = βˆ’1.

π‘₯β†’2+

(c) The one-sided limits limβˆ’ 𝑓 (π‘₯) and lim+ 𝑓 (π‘₯) do not agree. Therefore, the limit lim 𝑓 (π‘₯) does not exist, since 𝑓 (π‘₯) π‘₯β†’2

π‘₯β†’2

π‘₯β†’2

does not approach a single value as π‘₯ approaches 2 from both sides. (d) If we are looking at the behavior of 𝑓 (π‘₯) close to π‘₯ = 0, then we are looking at values of 𝑓 (π‘₯) for π‘₯ ≀ 2. So for values of π‘₯ near zero, 𝑓 (π‘₯) = 3π‘₯ βˆ’ 5. As π‘₯ approaches zero, 𝑓 (π‘₯) approaches 3(0) βˆ’ 5 = βˆ’5. Therefore, lim 𝑓 (π‘₯) = βˆ’5. π‘₯β†’0


136

Chapter One /SOLUTIONS

66. (a) When π‘₯ < 0, 𝑝(π‘₯) = π‘₯ + 3. So as π‘₯ approaches 0 from the left, 𝑝(π‘₯) approaches 0 + 3 = 3. Thus lim 𝑝(π‘₯) = 3.

π‘₯β†’0βˆ’

(b) When π‘₯ > 0, 𝑝(π‘₯) = π‘₯3 + 1. So as π‘₯ approaches 0 from the right, 𝑝(π‘₯) approaches 03 + 1 = 1. Thus lim 𝑝(π‘₯) = 1.

π‘₯β†’0+

(c) The left-hand and right-hand limits of 𝑝(π‘₯) at π‘₯ = 0 do not agree. Therefore, lim 𝑝(π‘₯) does not exist, since there is no π‘₯β†’0

single value that 𝑝(π‘₯) approaches as π‘₯ approaches 0 from both sides. (d) No matter what the value of 𝑑 is, 𝑑2 β‰₯ 0. So for all 𝑑, 𝑝(𝑑2 ) = (𝑑2 )3 + 1 = 𝑑6 + 1. So as 𝑑 approaches 0 from either side, 𝑝(𝑑2 ) approaches 06 + 1 = 1. Therefore, lim 𝑝(𝑑2 ) = 1. 𝑑→0

67. Evaluating

2

π‘₯ βˆ’ 25 at π‘₯ = 5 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯βˆ’5 (π‘₯ + 5)(π‘₯ βˆ’ 5) π‘₯2 βˆ’ 25 = . π‘₯βˆ’5 π‘₯βˆ’5

Since π‘₯ β‰  5 in the limit, we can cancel the common factor π‘₯ βˆ’ 5 to see lim π‘₯β†’5

68. Evaluating

(π‘₯ + 5)(π‘₯ βˆ’ 5) π‘₯2 βˆ’ 25 = lim = lim(π‘₯ + 5) = 10. π‘₯β†’5 π‘₯β†’5 π‘₯βˆ’5 π‘₯βˆ’5

π‘₯βˆ’4 at π‘₯ = 4 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯2 βˆ’ 16 π‘₯βˆ’4 π‘₯βˆ’4 = . (π‘₯ + 4)(π‘₯ βˆ’ 4) π‘₯2 βˆ’ 16

Since π‘₯ β‰  4 in the limit, we can cancel the common factor π‘₯ βˆ’ 4 to see lim

π‘₯βˆ’4

π‘₯β†’4 π‘₯2 βˆ’ 16

69. Evaluating

= lim

π‘₯βˆ’4

π‘₯β†’4 (π‘₯ + 4)(π‘₯ βˆ’ 4)

= lim

1

π‘₯β†’4 π‘₯ + 4

=

1 . 8

π‘₯2 βˆ’ 5π‘₯ + 6 at π‘₯ = 2 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯βˆ’2 (π‘₯ βˆ’ 3)(π‘₯ βˆ’ 2) π‘₯2 βˆ’ 5π‘₯ + 6 = . π‘₯βˆ’2 π‘₯βˆ’2

Since π‘₯ β‰  2 in the limit, we can cancel the common factor π‘₯ βˆ’ 2 to see lim π‘₯β†’2

70. Evaluating

(π‘₯ βˆ’ 3)(π‘₯ βˆ’ 2) π‘₯2 βˆ’ 5π‘₯ + 6 = lim = lim(π‘₯ βˆ’ 3) = βˆ’1. π‘₯β†’2 π‘₯β†’2 π‘₯βˆ’2 π‘₯βˆ’2

π‘₯βˆ’3 at π‘₯ = 3 gives us 0βˆ•0, so we see if we can rewrite the function using algebra. We have π‘₯2 + 2π‘₯ βˆ’ 15 π‘₯βˆ’3 π‘₯βˆ’3 = . (π‘₯ + 5)(π‘₯ βˆ’ 3) π‘₯2 + 2π‘₯ βˆ’ 15

Since π‘₯ β‰  3 in the limit, we can cancel the common factor π‘₯ βˆ’ 3 to see lim

π‘₯βˆ’3

π‘₯β†’3 π‘₯2 + 2π‘₯ βˆ’ 15

= lim

π‘₯βˆ’3

π‘₯β†’3 (π‘₯ + 5)(π‘₯ βˆ’ 3)

= lim

1

π‘₯β†’3 π‘₯ + 5

=

1 . 8

√ π‘₯2 + 8π‘₯ βˆ’ 2 is continuous everywhere on its domain (that is, at every point except π‘₯ = Β± 2.) In particular, 2 π‘₯ βˆ’2 it is continuous at π‘₯ = 2 so we find the limit by evaluating the expression at π‘₯ = 2. We have

71. The expression

18 π‘₯2 + 8π‘₯ βˆ’ 2 = = 9. π‘₯β†’2 2 π‘₯2 βˆ’ 2

lim


SOLUTIONS to Review Problems for Chapter One

137

72. Evaluating the expression at β„Ž = 0, we arrive at 0βˆ•0. Rewriting the expression using algebra gives lim

β„Žβ†’0

(4 + β„Ž)2 βˆ’ 42 (16 + 8β„Ž + β„Ž2 ) βˆ’ 16 = lim β„Žβ†’0 β„Ž β„Ž 8β„Ž + β„Ž2 = lim β„Žβ†’0 β„Ž β„Ž(8 + β„Ž) = lim β„Žβ†’0 β„Ž and since β„Ž β‰  0, canceling the common factor of β„Ž, we have = lim(8 + β„Ž) β„Žβ†’0

= 8.

PROBLEMS 73. (a) More fertilizer increases the yield until about 40 lbs.; then it is too much and ruins crops, lowering yield. (b) The vertical intercept is at π‘Œ = 200. If there is no fertilizer, then the yield is 200 bushels. (c) The horizontal intercept is at π‘Ž = 80. If you use 80 lbs. of fertilizer, then you will grow no apples at all. (d) The range is the set of values of π‘Œ attainable over the domain 0 ≀ π‘Ž ≀ 80. Looking at the graph, we can see that π‘Œ goes as high as 550 and as low as 0. So the range is 0 ≀ π‘Œ ≀ 550. (e) Looking at the graph, we can see that π‘Œ is decreasing near π‘Ž = 60. (f) Looking at the graph, we can see that π‘Œ is concave down everywhere, so it is certainly concave down near π‘Ž = 40. 74. (a) Given the two points (0, 32) and (100, 212), and assuming the graph in Figure 1.148 is a line, Slope =

180 212 βˆ’ 32 = = 1.8. 100 100

β—¦F

500 400 300 Boiling point of water

200 100

Freezing point of water

50 100 150 200 250

β—¦C

Figure 1.148 (b) The β—¦ F-intercept is (0, 32), so

β—¦

F = 1.8(β—¦ C) + 32.

β—¦

(c) If the temperature is 20 Celsius, then

β—¦

F = 1.8(20) + 32 = 68β—¦ F.

(d) If β—¦ F = β—¦ C, then β—¦

C = 1.8β—¦ C + 32

βˆ’32 = 0.8β—¦ C β—¦

C = βˆ’40β—¦ = β—¦ F.

75. (a) We have the following functions. (i) Since a change in 𝑝 of $5 results in a decrease in π‘ž of 2, the slope of π‘ž = 𝐷(𝑝) is βˆ’2βˆ•5 items per dollar. So 2 π‘ž = 𝑏 βˆ’ 𝑝. 5


138

Chapter One /SOLUTIONS Now we know that when 𝑝 = 550 we have π‘ž = 100, so 2 β‹… 550 5 100 = 𝑏 βˆ’ 220 100 = 𝑏 βˆ’

𝑏 = 320. Thus a formula is

2 π‘ž = 320 βˆ’ 𝑝. 5

(ii) We can solve π‘ž = 320 βˆ’ 25 𝑝 for 𝑝 in terms of π‘ž: 5π‘ž = 1600 βˆ’ 2𝑝 2𝑝 = 1600 βˆ’ 5π‘ž 5 𝑝 = 800 βˆ’ π‘ž. 2 The slope of this function is βˆ’5βˆ•2 dollars per item, as we would expect. 5 (b) A graph of 𝑝 = 800 βˆ’ π‘ž is given in Figure 1.149. 2 𝑝 (dollars) 800

550

100

320

π‘ž (items)

Figure 1.149 76. See Figure 1.150. 𝑑 (distance)

𝑑 (time)

Figure 1.150 77. (a)

(i) If the atoms are moved farther apart, then π‘Ÿ > π‘Ž so, from the graph, 𝐹 is negative, indicating an attractive force, which pulls the atoms back together. (ii) If the atoms are moved closer together, then π‘Ÿ < π‘Ž so, from the graph, 𝐹 is positive, indicating an attractive force, which pushes the atoms apart again. (b) At π‘Ÿ = π‘Ž, the force is zero. The answer to part (a)(i) tells us that if the atoms are pulled apart slightly, so π‘Ÿ > π‘Ž, the force tends to pull them back together; the answer to part (a)(ii) tells us that if the atoms are pushed together, so π‘Ÿ < π‘Ž, the force tends to push them back apart. Thus, π‘Ÿ = π‘Ž is a stable equilibrium.


SOLUTIONS to Review Problems for Chapter One

139

78. If the pressure at sea level is 𝑃0 , the pressure 𝑃 at altitude β„Ž is given by ) ( 0.4 β„Žβˆ•100 , 𝑃 = 𝑃0 1 βˆ’ 100 since we want the pressure to be multiplied by a factor of (1 βˆ’ 0.4βˆ•100) = 0.996 for each 100 feet we go up to make it decrease by 0.4% over that interval. At Mexico City β„Ž = 7340, so the pressure is 𝑃 = 𝑃0 (0.996)7340βˆ•100 β‰ˆ 0.745𝑃0 . So the pressure is reduced from 𝑃0 to approximately 0.745𝑃0 , a decrease of 25.5%. 79. Assuming the population of Ukraine is declining exponentially, we have population 𝑃 (𝑑) = 46.01π‘’π‘˜π‘‘ at time 𝑑 years after 2010. Using the 2014 population, we have 45.43 = 46.01π‘’βˆ’π‘˜β‹…4 ) ( 1 45.43 = 0.00317. π‘˜ = βˆ’ ln 4 46.01 We want to find the time 𝑑 at which 44 = 46.01π‘’βˆ’0.00317𝑑 ln(44βˆ•46.01) 𝑑=βˆ’ = 14.09 years. 0.00317 This model predicts the population to go below 44 million 14.09 years after 2010, in the year 2024. 80. (a) We compound the daily inflation rate 30 times to get the desired monthly rate π‘Ÿ: (

1+

π‘Ÿ 100

)1

) ( 0.67 30 = 1+ = 1.2218. 100

Solving for π‘Ÿ, we get π‘Ÿ = 22.18, so the inflation rate for April was 22.18%. (b) We compound the daily inflation rate 365 times to get a yearly rate 𝑅 for 2006: (

1+

𝑅 100

)1

) ( 0.67 365 = 1+ = 11.4426. 100

Solving for 𝑅, we get 𝑅 = 1044.26, so the yearly rate was 1044.26% during 2006. We could have obtained approximately the same result by compounding the monthly rate 12 times. Computing the annual rate from the monthly gives a lower result, because 12 months of 30 days each is only 360 days. 81. (a) The US consumption of hydroelectric power increased by at least 20% in 2011 and decreased by at least 10% in 2012, relative to each corresponding previous year. . (b) False. In 2012 hydroelectric power consumption increased only by 22.1% over consumption in 2011. (c) True. From 2011 to 2012 consumption decreased by 15.2%, which means π‘₯(1 βˆ’ 0.152) units of hydroelectric power were consumed in 2012 if π‘₯ had been consumed in 2011. Similarly, (π‘₯(1 βˆ’ 0.152)(1 βˆ’ 0.025) units of hydroelectric power were consumed in 2013 if π‘₯ had been consumed in 2012, and (π‘₯(1 βˆ’ 0.152)(1 βˆ’ 0.025)(1 βˆ’ 0.036) units of hydroelectric power were consumed in 2014 if π‘₯ had been consumed in 2013. Since π‘₯(1 βˆ’ 0.152)(1 βˆ’ 0.025)(1 βˆ’ 0.036) = π‘₯(0.797) = π‘₯(1 βˆ’ 0.203), the percent growth in hydroelectric power consumption was βˆ’20.3%, in 2014 relative to consumption in 2011. This amounts to about 20% decrease in hydroelectric power consumption from 2011 to 2014. 82. (a) For each 2.2 pounds of weight the object has, it has 1 kilogram of mass, so the conversion formula is π‘˜ = 𝑓 (𝑝) =

1 𝑝. 2.2

(b) The inverse function is 𝑝 = 2.2π‘˜, and it gives the weight of an object in pounds as a function of its mass in kilograms.


140

Chapter One /SOLUTIONS

83. Since 𝑓 (π‘₯) is a parabola that opens upward, we have 𝑓 (π‘₯) = π‘Žπ‘₯2 + 𝑏π‘₯ + 𝑐 with π‘Ž > 0. Since 𝑔(π‘₯) is a line with negative slope, 𝑔(π‘₯) = 𝑏 + π‘šπ‘₯, with slope π‘š < 0. Therefore 𝑔(𝑓 (π‘₯)) = 𝑏 + π‘š(π‘Žπ‘₯2 + 𝑏π‘₯ + 𝑐) = π‘šπ‘Žπ‘₯2 + π‘šπ‘π‘₯ + π‘šπ‘ + 𝑏. The coefficient of π‘₯2 is π‘šπ‘Ž, which is negative. Thus, the graph is a parabola opening downward. 84. (a) is 𝑔(π‘₯) since it is linear. (b) is 𝑓 (π‘₯) since it has decreasing slope; the slope starts out about 1 and then decreases to about 1 . (c) is β„Ž(π‘₯) since it has increasing slope; the slope starts out about 101 and then increases to about 1. 10 85. Given the doubling time of 2 hours, 200 = 100π‘’π‘˜(2) , we can solve for the growth rate π‘˜ using the equation: 2𝑃0 = 𝑃0 𝑒2π‘˜ ln 2 = 2π‘˜ ln 2 . π‘˜= 2 Using the growth rate, we wish to solve for the time 𝑑 in the formula ln 2

𝑃 = 100𝑒 2 𝑑 where 𝑃 = 3,200, so ln 2

3,200 = 100𝑒 2 𝑑 𝑑 = 10 hours. 86. (a) The 𝑦-intercept of 𝑓 (π‘₯) = π‘Ž ln(π‘₯ + 2) is 𝑓 (0) = π‘Ž ln 2. Since ln 2 is positive, increasing π‘Ž increases the 𝑦-intercept. (b) The π‘₯-intercept of 𝑓 (π‘₯) = π‘Ž ln(π‘₯ + 2) is where 𝑓 (π‘₯) = 0. Since this occurs where π‘₯ + 2 = 1, so π‘₯ = βˆ’1, increasing π‘Ž does not affect the π‘₯-intercept. 87. Since the factor by which the prices have increased after time 𝑑 is given by (1.05)𝑑 , the time after which the prices have doubled solves 2 = (1.05)𝑑 log 2 = log(1.05𝑑 ) = 𝑑 log(1.05) log 2 β‰ˆ 14.21 years. 𝑑= log 1.05 88. Using the exponential decay equation 𝑃 = 𝑃0 π‘’βˆ’π‘˜π‘‘ , we can solve for the substance’s decay constant π‘˜: (𝑃0 βˆ’ 0.3𝑃0 ) = 𝑃0 π‘’βˆ’20π‘˜ ln(0.7) π‘˜= . βˆ’20 Knowing this decay constant, we can solve for the half-life 𝑑 using the formula 0.5𝑃0 = 𝑃0 𝑒ln(0.7)π‘‘βˆ•20 20 ln(0.5) 𝑑= β‰ˆ 38.87 hours. ln(0.7) 89. (a) We know the decay follows the equation

𝑃 = 𝑃0 π‘’βˆ’π‘˜π‘‘ ,

and that 10% of the pollution is removed after 5 hours (meaning that 90% is left). Therefore, 0.90𝑃0 = 𝑃0 π‘’βˆ’5π‘˜ 1 π‘˜ = βˆ’ ln(0.90). 5 Thus, after 10 hours: 𝑃 = 𝑃0 π‘’βˆ’10((βˆ’0.2) ln 0.90) 𝑃 = 𝑃0 (0.9)2 = 0.81𝑃0 so 81% of the original amount is left.


SOLUTIONS to Review Problems for Chapter One

141

(b) We want to solve for the time when 𝑃 = 0.50𝑃0 : 0.50𝑃0 = 𝑃0 𝑒𝑑((0.2) ln 0.90) 0.2𝑑 )

0.50 = 𝑒ln(0.90

0.50 = 0.900.2𝑑 5 ln(0.50) 𝑑= β‰ˆ 32.9 hours. ln(0.90) 𝑃

(c) 𝑃0

5 10

𝑑

32.9

(d) When highly polluted air is filtered, there is more pollutant per liter of air to remove. If a fixed amount of air is cleaned every day, there is a higher amount of pollutant removed earlier in the process. 90. Since the amount of strontium-90 remaining halves every 29 years, we can solve for the decay constant; 0.5𝑃0 = 𝑃0 π‘’βˆ’29π‘˜ ln(1βˆ•2) π‘˜= . βˆ’29 Knowing this, we can look for the time 𝑑 in which 𝑃 = 0.10𝑃0 , or 0.10𝑃0 = 𝑃0 𝑒ln(0.5)π‘‘βˆ•29 29 ln(0.10) 𝑑= = 96.336 years. ln(0.5) 91. One hour. 92. (a) 𝑉0 represents the maximum voltage. (b) The period is 2πœ‹βˆ•(120πœ‹) = 1βˆ•60 second. (c) Since each oscillation takes 1βˆ•60 second, in 1 second there are 60 complete oscillations. 93. The US voltage has a maximum value of 156 volts and has a period of 1βˆ•60 of a second, so it executes 60 cycles a second. The European voltage has a higher maximum of 339 volts, and a slightly longer period of 1βˆ•50 seconds, so it oscillates at 50 cycles per second. 94. (a) The amplitude of the sine curve is |𝐴|. Thus, increasing |𝐴| stretches the curve vertically. See Figure 1.151. (b) The period of the wave is 2πœ‹βˆ•|𝐡|. Thus, increasing |𝐡| makes the curve oscillate more rapidlyβ€”in other words, the function executes one complete oscillation in a smaller interval. See Figure 1.152.

𝐴=3 𝐴=2 𝐴=1

-

R

3 2 1

βˆ’2πœ‹

𝐡=1

𝐡=2

𝑦

2πœ‹

𝑦 1

?

2πœ‹

π‘₯ βˆ’2πœ‹

βˆ’3

Figure 1.151

𝐡=3

βˆ’1

Figure 1.152

π‘₯


142

Chapter One /SOLUTIONS

95. (a)

(i) The water that has flowed out of the pipe in 1 second is a cylinder of radius π‘Ÿ and length 3 cm. Its volume is 𝑉 = πœ‹π‘Ÿ2 (3) = 3πœ‹π‘Ÿ2 . (ii) If the rate of flow is π‘˜ cm/sec instead of 3 cm/sec, the volume is given by 𝑉 = πœ‹π‘Ÿ2 (π‘˜) = πœ‹π‘Ÿ2 π‘˜. (i) The graph of 𝑉 as a function of π‘Ÿ is a quadratic. See Figure 1.153.

(b)

𝑉

𝑉

π‘Ÿ

π‘˜

Figure 1.153

Figure 1.154

(ii) The graph of 𝑉 as a function of π‘˜ is a line. See Figure 1.154. 96. Looking at 𝑔, we see that the ratio of the values is: 3.74 4.49 5.39 6.47 3.12 β‰ˆ β‰ˆ β‰ˆ β‰ˆ β‰ˆ 0.83. 3.74 4.49 5.39 6.47 7.76 Thus 𝑔 is an exponential function, and so 𝑓 and π‘˜ are the power functions. Each is of the form π‘Žπ‘₯2 or π‘Žπ‘₯3 , and since π‘˜(1.0) = 9.01 we see that for π‘˜, the constant coefficient is 9.01. Trial and error gives π‘˜(π‘₯) = 9.01π‘₯2 , since π‘˜(2.2) = 43.61 β‰ˆ 9.01(4.84) = 9.01(2.2)2 . Thus 𝑓 (π‘₯) = π‘Žπ‘₯3 and we find π‘Ž by noting that 𝑓 (9) = 7.29 = π‘Ž(93 ) so π‘Ž=

7.29 = 0.01 93

and 𝑓 (π‘₯) = 0.01π‘₯3 . 97. (a) See Figure 1.155. (b) The graph is made of straight line segments, rising from the π‘₯-axis at the origin to height π‘Ž at π‘₯ = 1, 𝑏 at π‘₯ = 2, and 𝑐 at π‘₯ = 3 and then returning to the π‘₯-axis at π‘₯ = 4. See Figure 1.156. 𝑦

𝑦 π‘Ž

4 3

βˆ’1

2

𝑐

1

𝑏 0

1

2

3

4

5

π‘₯

βˆ’1

0

Figure 1.155

1

2

3

4

5

π‘₯

Figure 1.156

98. (a) Reading the graph of πœƒ against 𝑑 shows that πœƒ β‰ˆ 5.2 when 𝑑 = 1.5. Since the coordinates of 𝑃 are π‘₯ = 5 cos πœƒ, 𝑦 = 5 sin πœƒ, when 𝑑 = 1.5 the coordinates are (π‘₯, 𝑦) β‰ˆ (5 cos 5.2, 5 sin 5.2) = (2.3, βˆ’4.4). (b) As 𝑑 increases from 0 to 5, the angle πœƒ increases from 0 to about 6.3 and then decreases to 0 again. Since 6.3 β‰ˆ 2πœ‹, this means that 𝑃 starts on the π‘₯-axis at the point (5, 0), moves counterclockwise the whole way around the circle (at which time πœƒ β‰ˆ 2πœ‹), and then moves back clockwise to its starting point.


SOLUTIONS to Review Problems for Chapter One

143

99. (a) III (b) IV (c) I (d) II 100. The functions 𝑦(π‘₯) = sin π‘₯ and π‘§π‘˜ (π‘₯) = π‘˜π‘’βˆ’π‘₯ for π‘˜ = 1, 2, 4, 6, 8, 10 are shown in Figure 1.157. The values of 𝑓 (π‘˜) for π‘˜ = 1, 2, 4, 6, 8, 10 are given in Table 1.19. These values can be obtained using either tracing or a numerical root finder on a calculator or computer. From Figure 1.157 it is clear that the smallest solution of sin π‘₯ = π‘˜π‘’βˆ’π‘₯ for π‘˜ = 1, 2, 4, 6 occurs on the first period of the sine curve. For small changes in π‘˜, there are correspondingly small changes in the intersection point. For π‘˜ = 8 and π‘˜ = 10, the solution jumps to the second period because sin π‘₯ < 0 between πœ‹ and 2πœ‹, but π‘˜π‘’βˆ’π‘₯ is uniformly positive. Somewhere in the interval 6 ≀ π‘˜ ≀ 8, 𝑓 (π‘˜) has a discontinuity.

2

π‘§π‘˜ (π‘₯) = π‘˜π‘’βˆ’π‘₯

+

1 0

6 2

4

Table 1.19

𝑦(π‘₯) = sin π‘₯

10

12

8

π‘₯

βˆ’1

Figure 1.157

π‘˜

𝑓 (π‘˜)

1

0.588

2

0.921

4

1.401

6

1.824

8

6.298

10

6.302

101. For any values of π‘˜, the function is continuous on any interval that does not contain π‘₯ = 2. Since 5π‘₯3 βˆ’ 10π‘₯2 = 5π‘₯2 (π‘₯ βˆ’ 2), we can cancel (π‘₯ βˆ’ 2) provided π‘₯ β‰  2, giving 𝑓 (π‘₯) =

5π‘₯3 βˆ’ 10π‘₯2 = 5π‘₯2 π‘₯βˆ’2

π‘₯ β‰  2.

Thus, if we pick π‘˜ = 5(2)2 = 20, the function is continuous. 102. At π‘₯ = 0, the curve 𝑦 = π‘˜ cos π‘₯ has 𝑦 = π‘˜ cos 0 = π‘˜. At π‘₯ = 0, the curve 𝑦 = 𝑒π‘₯ βˆ’ π‘˜ has 𝑦 = 𝑒0 βˆ’ π‘˜ = 1 βˆ’ π‘˜. If 𝑗(π‘₯) is continuous, we need 1 π‘˜ = 1 βˆ’ π‘˜, so π‘˜ = . 2 103. Two possible graphs are shown in Figures 1.158 and 1.159. velocity

distance

time

time

Figure 1.158: Velocity of the car

Figure 1.159: Distance

The distance moved by the car is continuous. (Figure 1.159 has no breaks in it.) In actual fact, the velocity of the car is also continuous; however, in this case, it is well-approximated by the function in Figure 1.158, which is not continuous on any interval containing the moment of impact. 104. Figure 1.160 suggests that as 𝑑 β†’ ∞, 3 βˆ’ 2π‘’βˆ’π‘‘ β†’ 3. We shall use limit properties to confirm this. We now calculate the limit in stages using the properties to justify each step: lim (3 βˆ’ 2π‘’βˆ’π‘‘ ) = lim (3) + lim (βˆ’2π‘’βˆ’π‘‘ )

(Property 2)

= lim (3) βˆ’ 2 lim (π‘’βˆ’π‘‘ )

(Property 1)

π‘‘β†’βˆž

π‘‘β†’βˆž π‘‘β†’βˆž

π‘‘β†’βˆž

π‘‘β†’βˆž

= 3 βˆ’ 2(0) = 3

(Property 6 and because π‘’βˆ’π‘‘ β†’ 0)


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