1.1 SOLUTIONS
1
CHAPTER ONE Solutions for Section 1.1 EXERCISES 1. Since π‘ represents the number of years since 2020, we see that π (5) represents the population of the city in 2025. In 2025, the cityβs population is 8 million. 2. Since π = π (π ), we see that π (200) is the value of π when π = 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 ο¬rst, 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 ineο¬ciency inherent in large organizations or simply to workers getting in each otherβs 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 β 0)β(1 β 0) = 1. So the equation of the line is π¦ = π₯. 7. The slope is (3 β 2)β(2 β 0) = 1β2. So the equation of the line is π¦ = (1β2)π₯ + 2. 8. The slope is
2 1 3β1 = = . 2 β (β2) 4 2 Now we know that π¦ = (1β2)π₯ + π. Using the point (β2, 1), we have 1 = β2β2 + π, which yields π = 2. Thus, the equation of the line is π¦ = (1β2)π₯ + 2. 6β0 9. The slope is = 2 so the equation of the line is π¦ β 6 = 2(π₯ β 2) or π¦ = 2π₯ + 2. 2 β (β1) 5 5 10. Rewriting the equation as π¦ = β π₯ + 4 shows that the slope is β and the vertical intercept is 4. 2 2 11. Rewriting the equation as 2 12 π¦=β π₯+ 7 7 shows that the line has slope β12β7 and vertical intercept 2β7. Slope =
12. Rewriting the equation of the line as β2 π₯β2 4 1 π¦ = π₯ + 2, 2
βπ¦ =
we see the line has slope 1β2 and vertical intercept 2.
2
Chapter One /SOLUTIONS 13. Rewriting the equation of the line as 12 4 π₯β 6 6 2 π¦ = 2π₯ β , 3 π¦=
we see that the line has slope 2 and vertical intercept β2β3. 14. The intercepts appear to be (0, 3) and (7.5, 0), giving Slope =
6 2 β3 =β =β . 7.5 15 5
The π¦-intercept is at (0, 3), so a possible equation for the line is 2 π¦ = β π₯ + 3. 5 (Answers may vary.) 15. π¦ β π = π(π₯ β π) 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 β 27.8 1.4 = = 14. 5.3 β 5.2 0.1
Using the point-slope formula, with the point (5.2, 27.8), we get the equation π¦ β 27.8 = 14(π₯ β 5.2) which is equivalent to π¦ = 14π₯ β 45. 17. π¦ = 5π₯ β 3. Since the slope of this line is 5, we want a line with slope β 15 passing through the point (2, 1). The equation is (π¦ β 1) = β 15 (π₯ β 2), or π¦ = β 15 π₯ + 75 .
18. The line π¦ + 4π₯ = 7 has slope β4. Therefore the parallel line has slope β4 and equation π¦ β 5 = β4(π₯ β 1) or π¦ = β4π₯ + 9. β1 = 14 and equation π¦ β 5 = 14 (π₯ β 1) or π¦ = 0.25π₯ + 4.75. The perpendicular line has slope (β4) 19. The line parallel to π¦ = ππ₯ + π also has slope π, so its equation is π¦ = π(π₯ β π) + π. The line perpendicular to π¦ = ππ₯ + π has slope β1βπ, so its equation will be 1 π¦ = β (π₯ β π) + π. π 20. Since the function goes from π₯ = 0 to π₯ = 4 and between π¦ = 0 and π¦ = 2, the domain is 0 β€ π₯ β€ 4 and the range is 0 β€ π¦ β€ 2. 21. Since π₯ goes from 1 to 5 and π¦ goes from 1 to 6, the domain is 1 β€ π₯ β€ 5 and the range is 1 β€ π¦ β€ 6. 22. Since the function goes from π₯ = β2 to π₯ = 2 and from π¦ = β2 to π¦ = 2, the domain is β2 β€ π₯ β€ 2 and the range is β2 β€ π¦ β€ 2. 23. Since the function goes from π₯ = 0 to π₯ = 5 and between π¦ = 0 and π¦ = 4, the domain is 0 β€ π₯ β€ 5 and the range is 0 β€ π¦ β€ 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 < π¦ β€
1 . 2
1.1 SOLUTIONS
3
26. The value of π (π‘) is real provided π‘2 β 16 β₯ 0 or π‘2 β₯ 16. This occurs when either π‘ β₯ 4, or π‘ β€ β4. Solving π (π‘) = 3, we have β π‘2 β 16 = 3 π‘2 β 16 = 9 π‘2 = 25 so π‘ = Β±5. 27. We have π = ππ3 . You may know that π = π . π‘ 29. For some constant π, we have π = πβ2 .
4 3 ππ . 3
28. If distance is π, then π£ =
30. We know that πΈ is proportional to π£3 , so πΈ = ππ£3 , for some constant π. 31. We know that π is proportional to 1βπ2 , so π=
π , π2
for some constant π.
PROBLEMS 32. (a) Each date, π‘, has a unique daily snowfall, π, 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: π (thousand dollars)
(5, 6)
π (years)
Figure 1.1 (c) The vertical intercept is the value of π when π = 0, or the value of the car when it is new. The horizontal intercept is the value of π when π = 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 ο¬at 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 ο¬rst 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 π‘ = 2. Thus, an expression that represents the statement is: π (2) = 7.088.
4
Chapter One /SOLUTIONS 36. The year 2020 was 0 years before 2020 so 2020 corresponds to π‘ = 0. Thus, an expression that represents the statement is: π (0) meters. 37. The year 1949 was 2020 β 1949 = 71 years before 2020 so 1949 corresponds to π‘ = 71. Similarly, we see that the year 2000 corresponds to π‘ = 20. Thus, an expression that represents the statement is: π (71) = π (20). 38. The year 2018 was 2 years before 2020 so 2018 corresponds to π‘ = 2. Similarly, π‘ = 3 corresponds to the year 2017. Thus, π (3) and π (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, π (2), is 0.011 less than the sea level in 2017 which is π (3). An expression that represents the statement is: π (2) = π (3) β 0.011. Note that there are other possible equivalent expressions, such as: π (2) β π (3) = β0.011. 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
5
42. See Figure 1.5. distance between cars
distance driven
Figure 1.5 43. (a) π (30) = 10 means that the value of π at π‘ = 30 was 10. In other words, the temperature at time π‘ = 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 measures the value of π (π‘) when π‘ = 0. In other words, when the object was initially put outside, it had a temperature of πβ¦ C. The intercept π measures the value of π‘ when π (π‘) = 0. In other words, at time π the objectβs 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. π (meters)
π‘ (sec)
Figure 1.6 (b) The statement π (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 π when π‘ = 0; that is, the height from which the rock is dropped. The horizontal intercept is the value of π‘ when π = 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 β 6.75 = 0.4 . 2006 β 1992 year
(b) With π‘ as the year and π (π‘) as the quantity of imports in millions of barrels per day, we have π (π‘) = 6.75 + 0.4(π‘ β 1992). Alternatively, if π‘ is the number of years since 1992 and if π (π‘) is the quantity of imports in millions of barrels per day π (π‘) = 6.75 + 0.4π‘.
6
Chapter One /SOLUTIONS (c) We have 6.75 + 0.4π‘ = 18 π‘ = 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 = 100 mm corresponds to about π = 600 kgβhectare, and π = 600 mm corresponds to about π = 5800 kgβhectare. Using a diο¬erence quotient we have Ξπ 5800 β 600 = = 10.4 kgβhectare per mm. Ξπ 600 β 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 =
π = π + 10.4π. Substituting π = 100 and π = 600 we can solve for π. π + 10.4(100) = 600 π = β440. The equation of the line is π = β440 + 10.4π. 48. (a) Reading coordinates from the graph, we see that rainfall π = 100 mm corresponds to about π = 300 kgβhectare, and π = 600 mm corresponds to about π = 3200 kgβhectare. Using a diο¬erence quotient we have Ξπ 3200 β 300 = = 5.8 kgβhectare per mm. Ξπ 600 β 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 =
π = π + 5.8π. Substituting π = 100 and π = 300 we can solve for π. π + 5.8(100) = 300 π = β280. The equation of the line is π = β280 + 5.8π. 49. The diο¬erence quotient ΞπβΞπ 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 π(π‘): π(10) = 300 + 1.4 β (10) = 314 ppm π(20) = 300 + 1.4 β (20) = 328 ppm π(100) = 300 + 1.4 β (100) = 440 ppm (b) Substituting into β(π‘): β(10) = 300 + 1.5 β (10) = 315 ppm β(20) = 300 + 1.5 β (20) = 330 ppm β(100) = 300 + 1.5 β (100) = 450 ppm (c) They diο¬er in slope, 1.4 vs. 1.5 ppm per year. This creates a larger diο¬erence between π(π‘) and β(π‘) for larger values of π‘: For π‘ = 10, the diο¬erence is β(10) β π(10) = 315 β 314 = 1 ppm. For π‘ = 100, the diο¬erence is β(100) β π(100) = 450 β 440 = 10 ppm.
1.1 SOLUTIONS
7
51. (a) Let π₯ be the average minimum daily temperature (β¦ C), and let π¦ be the date the marmot is ο¬rst sighted. Reading coordinates from the graph, we see that temperature π₯ = 12β¦ C corresponds to date π¦ = 137 days after Jan 1, and π₯ = 22β¦ C corresponds to π¦ = 109 days. Using a diο¬erence quotient, we have days Ξπ¦ 109 β 137 = = β2.8 β¦ . Ξπ₯ 22 β 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 Ξπ¦ = Slope Γ Ξπ₯ = (β2.8)(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 =
π¦ = π β 2.8π₯. Substituting π₯ = 12 and π¦ = 137 we solve for π. π β 2.8(12) = 137 π = 171. The equation of the line is π¦ = 171 β 2.8π₯. 52. (a) If the ο¬rst date of bare ground is 140, then, according to the ο¬gure, the ο¬rst bluebell ο¬ower is sighted about day 150, that is 150 β 140 = 10 days later. (b) Let π₯ be the ο¬rst date of bare ground, and let π¦ be the date the ο¬rst bluebell ο¬ower is sighted. Reading coordinates from the graph, we see that date π₯ = 130 days after Jan 1 corresponds to date π¦ = 142 days after Jan 1, and π₯ = 170 days corresponds to π¦ = 173 days. Using a diο¬erence quotient we have Ξπ¦ 173 β 142 = = 0.775 days per day. Ξπ₯ 170 β 130 (c) The slope is positive, so an increase in the π₯-variable corresponds to an increase in the π¦-variable. These variables represents days in the year, and larger values indicate days that are later in the year. Thus if bare ground ο¬rst occurs later in the year, then bluebells ο¬rst ο¬ower later in the year. Positive slope means that bluebells ο¬ower later when the snow cover lasts longer. (d) Using the slope, we see that the equation has the form Slope =
π¦ = π + 0.775π₯. Substituting π₯ = 130 and π¦ = 142 we can solve for π. π + 0.775(130) = 142 π = 41.25. The equation of the line is π¦ = 41.25 + 0.775π₯. 53. (a) We have π =
256 = 14.222 cm per hour. When the snow started, there were 100 cm on the ground, so 18 π (π‘) = 100 + 14.222π‘.
(b) The domain of π is 0 β€ π‘ β€ 18 hours. The range is 100 β€ π (π‘) β€ 356 cm. 54. (a) We ο¬nd the slope π and intercept π in the linear equation πΆ = π + ππ€. To ο¬nd the slope π, we use π=
ΞπΆ 1098.32 β 694.55 = = 134.59 dollars per ton. Ξπ€ 8β5
We substitute to ο¬nd π: πΆ = π + ππ€ 694.55 = π + (134.59)(5) π = 21.6 dollars. The linear formula is πΆ = 21.6 + 134.59π€. (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 ο¬at fee for waste collection is $21.60. This is the amount charged even if there is no waste.
8
Chapter One /SOLUTIONS
55. We are looking for a linear function π¦ = π (π₯) that, given a time π₯ in years, gives a value π¦ in dollars for the value of the refrigerator. We know that when π₯ = 0, that is, when the refrigerator is new, π¦ = 950, and when π₯ = 7, the refrigerator is worthless, so π¦ = 0. Thus (0, 950) and (7, 0) are on the line that we are looking for. The slope is then given by 950 β7 It is negative, indicating that the value decreases as time passes. Having found the slope, we can take the point (7, 0) and use the point-slope formula: π¦ β π¦1 = π(π₯ β π₯1 ). So, 950 (π₯ β 7) π¦β0 = β 7 950 π₯ + 950. π¦=β 7 π=
55 β 40 Ξ$ = = $0.025/cu. ft. 56. (a) Charge per cubic foot = Ξ cu. ft. 1600 β 1000 Alternatively, if we let π = cost, π€ = cubic feet of water, π = ο¬xed charge, and π = cost/cubic feet, we obtain π = π + ππ€. Substituting the information given in the problem, we have 40 = π + 1000π 55 = π + 1600π. Subtracting the ο¬rst equation from the second yields 15 = 600π, so π = 0.025. (b) The equation is π = π + 0.025π€, so 40 = π + 0.025(1000), which yields π = 15. Thus the equation is π = 15 + 0.025π€. (c) We need to solve the equation 100 = 15 + 0.025π€, which yields π€ = 3400. It costs $100 to use 3400 cubic feet of water. 57. (a) The ο¬rst companyβs price for a dayβs rental with π miles on it is πΆ1 (π) = 40 + 0.15π. Its competitorβs price for a dayβs rental with π miles on it is πΆ2 (π) = 50 + 0.10π. (b) See Figure 1.8. πΆ (cost in dollars) πΆ1 (π) = 40 + 0.15π
150 100
πΆ2 (π) = 50 + 0.10π
50 0
200
400
600
800
π (miles)
Figure 1.8 (c) To ο¬nd which company is cheaper, we need to determine where the two lines intersect. We let πΆ1 = πΆ2 , and thus 40 + 0.15π = 50 + 0.10π 0.05π = 10 π = 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 ο¬rst company is cheaper. 58. (a) We ο¬nd the slope π and intercept π in the linear equation π = π + ππ‘. To ο¬nd the slope π, we use 66 β 113 Ξπ = = β0.94. Ξπ‘ 50 β 0 When π‘ = 0, we have π = 113, so the intercept π is 113. The linear formula is π=
π = 113 β 0.94π‘. (b) We use the formula π = 113 β 0.94π‘. When π = 20, we have 20 = 113 β 0.94π‘ and so π‘ = 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) π (2001) = 272 (ii) π (2019) = 607 (b) The average yearly increase is the rate of change. Yearly increase =
π (2019) β π (2001) 607 β 272 335 = = = 18.611 billionaires per year. 2019 β 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 335β18 = 18.611 billionaires per year. The equation is 335 π‘ π (π‘) = π + 18 where π (2001) = 272, so 335 (2001) 272 = π + 18 π = β36,968.833. Thus, π (π‘) = 18.611π‘ β 36,968.833. 60. (a) The variable costs for π₯ acres are $200π₯, or 0.2π₯ thousand dollars. The total cost, πΆ (again in thousands of dollars), of planting π₯ acres is: πΆ = π (π₯) = 10 + 0.2π₯. This is a linear function. See Figure 1.9. Since πΆ = π (π₯) increases with π₯, π is an increasing function of π₯. Look at the values of πΆ shown in the table; you will see that each time π₯ increases by 1, πΆ increases by 0.2. Because πΆ increases at a constant rate as π₯ increases, the graph of πΆ against π₯ is a line. (b) See Figure 1.9 and Table 1.1. Table 1.1 Cost of planting seed π₯
πΆ
0
10
2
10.4
3
10.6
4
10.8
5
11
6
11.2
πΆ (thosand $) 10
πΆ = 10 + 0.2π₯
5
2
4
6
π₯ (acres)
Figure 1.9
(c) The vertical intercept of 10 corresponds to the ο¬xed costs. For πΆ = π (π₯) = 10 + 0.2π₯, the intercept on the vertical axis is 10 because πΆ = π (0) = 10 + 0.2(0) = 10. Since 10 is the value of πΆ when π₯ = 0, we recognize it as the initial outlay for equipment, or the ο¬xed 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 π (π₯) = 10 + 0.2π₯. 61. We will let π = amount of fuel for take-oο¬, πΏ = amount of fuel for landing, π = amount of fuel per mile in the air, π = the length of the trip in miles. Then π, the total amount of fuel needed, is given by π(π) = π + πΏ + π π.
10
Chapter One /SOLUTIONS
62. (a) The scale of the graph makes it impossible to read values of π (423) and π (422) accurately enough to evaluate their diο¬erence. But that diο¬erence equals the slope of the line, which we can estimate. Using the points (400, 2000) and (600, 6000) on the line, we have 6000 β 2000 = 20. Slope = 600 β 400 Thus π (423) β π (422) = 20. (b) We have Ξπ¦ = Slope Γ Ξπ₯ = (20)(517 β 513) = 80. Thus π (517) β π (513) = 80. 63. (a) The scale of the graph makes it impossible to read values of π(4210) and π(4209) accurately enough to evaluate their diο¬erence. But that diο¬erence equals the slope of the line, which we can estimate. Using the points (3000, 70) and (5000, 50) on the line, we have 50 β 70 = β0.01. Slope = 5000 β 3000 So Ξπ¦ = Slope Γ Ξπ₯ = (β0.01)(4210 β 4209) = β0.01. Thus π(4210) β π(4209) = β0.01. (b) We have Ξπ¦ = Slope Γ Ξπ₯ = (β0.01)(3760 β 3740) = β0.2. Thus π(3760) β π(3740) = β0.2. 64. (a) From the graph we estimate π (1) = 100 mph and π (2) = 50 mph. (b) No. Counterexample with π‘ = 1: π (π‘ + 1) = π (2) = 50 π (π‘) + 1 = π (1) + 1 = 100 + 1 = 101. (c) No. Counterexample with π‘ = 1: π (π‘ + 1) = 50 π (π‘) + π (1) = 100 + 100 = 200. 65. (a) From the graph we estimate π(1) = 50% and π(2) = 75%. (b) No. Counterexample with π‘ = 1: π(π‘ + 1) = π(2) = 75 π(π‘) + 1 = π(1) + 1 = 50 + 1 = 51. (c) No. Counterexample with π‘ = 1: π(π‘ + 1) = 75 π(π‘) + π(1) = 50 + 50 = 100. 66. (a) The largest time interval was 2016β2018 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 2012β2014 and in 2015β2016.) (b) The largest time interval was 2015β2018 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 2015β2017 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 2012β2015 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 2008β2010 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 2009β2010 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 π‘ = 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 ο¬ve 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 π‘ = 125). Similar reasoning yields Table 1.2. Table 1.2 Year
1889
1914
1939
1964
1989
2014
π
6.900
6.985
6.964
6.990
7.083
7.071
70. (a) This could be a linear function because π€ increases by 2.7 as β increases by 4. (b) We ο¬nd the slope π and the intercept π in the linear equation π€ = π + πβ. We ο¬rst ο¬nd the slope π using the ο¬rst two points in the table. Since we want π€ to be a function of β, we take π=
82.4 β 79.7 Ξπ€ = = 0.68. Ξβ 172 β 168
Substituting the ο¬rst point and the slope π = 0.68 into the linear equation π€ = π+πβ, we have 79.7 = π+(0.68)(168), so π = β34.54. The linear function is π€ = 0.68β β 34.54. The slope, π = 0.68, is in units of kg per cm. (c) We ο¬nd the slope and intercept in the linear function β = π + ππ€ using π = ΞββΞπ€ to obtain the linear function β = 1.47π€ + 50.79. Alternatively, we could solve the linear equation found in part (b) for β. The slope, π = 1.47, has units cm per kg. 71. (a) Since the diο¬erences in π -values are constant (Ξπ = 147) for equally spaced β-values (Ξβ = 2), π could be a linear function of β. (b) To ο¬nd a formula for π = π (β), we ο¬rst ο¬nd the slope: Ξπ 147 = = 73.5 torr per meter. Ξπ‘ 2 Thus, the equation of the line has the form π = 73.5β + π, where π is the vertical intercept. To ο¬nd π, we choose a point from the table: for example, when β = 6, we have π = 1201. Substituting these values, we have π = 73.5β + π 1201 = 73.5(6) + π π = 1201 β 73.5(6) = 760. Therefore, π = π (β) = 73.5β + 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 π (0) = 760 torr. Since we want the value of β when the pressure is twice that at the surface, we solve π (β) = 2 β 760: 2 β 760 = π (β) 1520 = 73.5β + 760 73.5β = 760 760 = 10.34. β= 73.5
72. (a) Since the initial value is $25,000 and the slope is β2000, the value of the vehicle at time π‘ is π (π‘) = 25000 β 2000π‘. The cost of repairs has initial value 0 and slope 1500, so πΆ(π‘) = 1500π‘. Figure 1.10 shows the graphs of these two functions. dollars 25000 π (π‘)
20000
πΆ(π‘)
15000 10000 5000 0
2
4
6
8
10
12
π‘ (years)
Figure 1.10 (b) The vehicle value equals the repair cost, when π (π‘) = πΆ(π‘). 25000 β 2000π‘ = 1500π‘ 25000 = 3500π‘ 7.143 = π‘. Thus, replace during the eighth year (because the ο¬rst year ends at π‘ = 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 π (π‘) = 1500. 25000 β 2000π‘ = 1500 25000 = 1500 + 2000π‘ 23500 = 2000π‘ 11.750 = π‘. Thus, in the twelfth year (because the ο¬rst year ends at π‘ = 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 π(π) is negative. If the owner increases the price, she is willing to make more cakes. Thus the slope of π (π) is positive. (b) To determine whether an ordered pair (π, π) is a solution to the inequality, we substitute the values of π and π into the inequality and see whether the resulting statement is true. Substituting the two ordered pairs gives (60, 18):
18 β€ 20 β 60β20, or 18 β€ 17.
This is false, so (60, 18) is not a solution.
(120, 12): 12 β€ 20 β 120β20, or 12 β€ 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 π β€ 20 β πβ20. 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, π) represents a quantity of cakes π that customers would be willing to buy at the unit price π. (c) In order to be a solution to both of the given inequalities, a point (π, π) must lie on or below the line π = 20 β πβ20 and on or above the line π = 11 + πβ40. Thus, the solution set of the given system of inequalities is the region shaded in Figure 1.11. A point (π, π) in this region represents a quantity π of cakes that customers would be willing to buy, and that the bakery-owner would be willing to make and sell, at the price π. π 25 20
π(π) = 20 β πβ20 (120, 14)
15 10
π (π) = 11 + πβ40
5 40
80
120
160
200
π
Figure 1.11: Possible cake sales at diο¬erent prices and quantities (d) To ο¬nd the rightmost point of this region, we need to ο¬nd the intersection point of the lines π = 20 β πβ20 and π = 11 + πβ40. At this point, π is equal to both 20 β πβ20 and 11 + πβ40, so these two expressions are equal to each other: π π = 11 + 20 β 20 40 π π 9= + 20 40 3π 9= 40 π = 120. Therefore, π = 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 π = 20 β 120β20 = 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.) = β1 and π¦-intercept 2, so its equation is 74. (a) The line given by (0, 2) and (1, 1) has slope π = 2β1 β1 π¦ = βπ₯ + 2. The points of intersection of this line with the parabola π¦ = π₯2 are given by π₯2 = βπ₯ + 2 π₯2 + π₯ β 2 = 0 (π₯ + 2)(π₯ β 1) = 0. The solution π₯ = 1 corresponds to the point we are already given, so the other solution, π₯ = β2, gives the π₯-coordinate of πΆ. When we substitute back into either equation to get π¦, we get the coordinates for πΆ, (β2, 4). = 1 β π, and π¦-intercept at (0, π), so we can write the equation (b) The line given by (0, π) and (1, 1) has slope π = πβ1 β1 for the line as we did in part (a): π¦ = (1 β π)π₯ + π. We then solve for the points of intersection with π¦ = π₯2 the same way: π₯2 = (1 β π)π₯ + π 2
π₯ β (1 β π)π₯ β π = 0 π₯2 + (π β 1)π₯ β π = 0 (π₯ + π)(π₯ β 1) = 0
14
Chapter One /SOLUTIONS Again, we have the solution at the given point (1, 1), and a new solution at π₯ = βπ, corresponding to the other point of intersection πΆ. Substituting back into either equation, we can ο¬nd the π¦-coordinate for πΆ is π2 , and thus πΆ is given by (βπ, π2 ). This result agrees with the particular case of part (a) where π = 2.
75. Looking at the given data, it seems that Galileoβs hypothesis was incorrect. The ο¬rst 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 functionβs rise (Ξπ¦) over its run (Ξπ₯) over any interval. So, for π¦ = π+ππ₯, we have: Ξπ¦ . Slope = π = Ξπ₯ 77. The line π₯ = 3 is vertical, so it is not a function of π₯: it fails the vertical line test. The line π¦ = 3 is horizontal, hence a linear function of π₯ with slope 0. 78. The line π¦ β 3 = 0 or, equivalently, π¦ = 3 is horizontal, hence has slope 0 in the π₯π¦-plane. 79. The line π¦ = 0.5 β 3π₯ has a negative slope and is therefore a decreasing function. 80. If π¦ is directly proportional to π₯ we have π¦ = ππ₯. Adding the constant 1 to give π¦ = 2π₯ + 1 means that π¦ is not proportional to π₯. 81. One possible answer is π (π₯) = 2π₯ + 3. 8 82. One possible answer is π = 1β3 . π 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 π¦ = π + ππ₯, the corresponding values of π¦ are π + ππ₯1 and π + π(π₯1 + 1). Thus π¦ increases by Ξπ¦ = π + π(π₯1 + 1) β (π + ππ₯1 ) = π. 85. True. Solving for π¦ on the second equation, we see that the second linear function has the same equation as the ο¬rst: π₯ = βπ¦ + 1 π₯ β 1 = βπ¦ βπ₯ + 1 = π¦. 86. False. Solving for π¦ on the second equation, we get π¦ = (β1β2)π₯ + 1 which is a linear function with a diο¬erent slope and intercept from the ο¬rst equation. 87. False. For example, let π¦ = 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 diο¬erent. The ratio π¦βπ₯ is constant for linear functions of the form π¦ = ππ₯, but not in general. (Other examples are possible.) 88. False. For example, if π¦ = 4π₯ + 1 (so π = 4) and π₯ = 1, then π¦ = 5. Increasing π₯ by 2 units gives 3, so π¦ = 4(3) + 1 = 13. Thus, π¦ has increased by 8 units, not 4 + 2 = 6. (Other examples are possible.) β 89. (b) and (c). For π(π₯) = π₯, the domain and range are all nonnegative numbers, and for β(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 = β0.08 = β8% (decay). 7. Initial quantity = 3.2; growth rate = 0.03 = 3% (continuous). 8. Initial quantity = 15; growth rate = β0.06 = β6% (continuous decay). ( )π‘ 9. Since π0.25π‘ = π0.25 β (1.2840)π‘ , we have π = 15(1.2840)π‘ . This is exponential growth since 0.25 is positive. We can also see that this is growth because 1.2840 > 1. 10. Since πβ0.5π‘ = (πβ0.5 )π‘ β (0.6065)π‘ , we have π = 2(0.6065)π‘ . This is exponential decay since β0.5 is negative. We can also see that this is decay because 0.6065 < 1. 11. π = π0 (π0.2 )π‘ = π0 (1.2214)π‘ . Exponential growth because 0.2 > 0 or 1.2214 > 1. 12. π = 7(πβπ )π‘ = 7(0.0432)π‘ . Exponential decay because βπ < 0 or 0.0432 < 1. 13. (a) Let π = π0 ππ‘ . Then π0 π5 = 75.94 and π0 π7 = 170.86. So π0 π7 170.86 = = 2.25 = π2 . 75.94 π0 π5 So π = 1.5. (b) Since π = 1.5, the growth rate is π = 0.5 = 50%. 14. (a) Let π = π0 ππ‘ . Then π0 π0.02 = 25.02 and π0 π0.05 = 25.06. So π0 π0.05 25.06 = = 1.001 = π0.03 . 25.02 π0 π0.02 So
100
π = (1.001) 3 = 1.05. (b) Since π = 1.05, the growth rate is π = 0.05 = 5%. 15. (a) The function is linear with initial population of 1000 and slope of 50, so π = 1000 + 50π‘. (b) This function is exponential with initial population of 1000 and growth rate of 5%, so π = 1000(1.05)π‘ . 16. (a) This is a linear function with slope β2 grams per day and intercept 30 grams. The function is π = 30 β 2π‘, and the graph is shown in Figure 1.12. π (grams)
π (grams)
30
30 π = 30 β 2π‘
15
Figure 1.12
π = 30(0.88)π‘
π‘ (days)
15
π‘ (days)
Figure 1.13
(b) Since the quantity is decreasing by a constant percent change, this is an exponential function with base 1β0.12 = 0.88. The function is π = 30(0.88)π‘ , and the graph is shown in Figure 1.13. 17. The function is increasing and concave up between π· and πΈ, and between π» and πΌ. It is increasing and concave down between π΄ and π΅, and between πΈ and πΉ . It is decreasing and concave up between πΆ and π·, and between πΊ and π». Finally, it is decreasing and concave down between π΅ and πΆ, and between πΉ and πΊ 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 ο¬xed quantity. While β(π₯) decreases by 3 whenever π₯ increases by 1, π (π₯) and π(π₯) fail this test, since both change by diο¬erent amounts between π₯ = β2 and π₯ = β1 and between π₯ = β1 and π₯ = 0. So the only possible linear function is β(π₯), so it will be given by a formula of the type: β(π₯) = ππ₯ + π. As noted, π = β3. Since the π¦-intercept of β is 31, the formula for β(π₯) is β(π₯) = 31 β 3π₯. (b) An exponential function must grow by exactly the same factor whenever π₯ changes by some ο¬xed quantity. Here, π(π₯) increases by a factor of 1.5 whenever π₯ increases by 1. Since the π¦-intercept of π(π₯) is 36, π(π₯) has the formula π(π₯) = 36(1.5)π₯ . The other two functions are not exponential; β(π₯) is not because it is a linear function, and π (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 π¦ = 2.2 because all π¦ values are the same. Table B could represent a linear function of π₯ with slope equal to 11β4. This is because π₯ values that diο¬er by 4 have corresponding π¦ values that diο¬er by 11, and π₯ values that diο¬er by 8 have corresponding π¦ values that diο¬er by 22. In Table C, π¦ 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 π¦ values is the same for all equally spaced π₯ values. Thus, the π¦ 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 π¦ values corresponding to equally spaced π₯ values is not the same. In Table C, π¦ decreases and then increases as π₯ increases. So neither Table B nor Table C can represent exponential functions. 22. Since π is linear, its slope is a constant π=
20 β 10 = 5. 2β0
Thus π increases 5 units for unit increase in π₯, so π (1) = 15,
π (3) = 25,
π (4) = 30.
Since π is exponential, its growth factor is constant. Writing π(π₯) = πππ₯ , we have π(0) = π = 10, so π(π₯) = 10 β ππ₯ . Since π(2) = 10 β π2 = 20, we have π2 = 2 and since π > 0, we have β π = 2. β Thus π increases by a factor of 2 for unit increase in π₯, so β β β π(1) = 10 2, π(3) = 10( 2)3 = 20 2,
β π(4) = 10( 2)4 = 40.
Notice that the value of π(π₯) doubles between π₯ = 0 and π₯ = 2 (from π(0) = 10 to π(2) = 20), so the doubling time of π(π₯) is 2. Thus, π(π₯) doubles again between π₯ = 2 and π₯ = 4, conο¬rming that π(4) = 40. 23. We see that 1.09 β 1.03, and therefore β(π ) = π(1.03)π ; π must be 1. Similarly 2.42 = 1.1, and so π (π ) = π(1.1)π ; π = 2. 1.06 2.20 Lastly, 3.65 β 1.05, so π(π ) = π(1.05)π ; π β 3. 3.47
24. (a) This is the graph of a linear function, which increases at a constant rate, and thus corresponds to π(π‘), 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(π‘), 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 π(π‘), whose increases are 1, 2, 3, 4, and 5. 25. (a) This is a linear function, corresponding to π(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(π₯). (The rates are β0.2, β0.3, β0.4, β0.5, β0.6.) (c) This graph is concave up, so it corresponds to a function whose rate of decrease is decreasing, like π (π₯). (The rates are β10, β9, β8, β7, β6.)
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 π = 50(1.4)π‘ and graph (II) is π = 50(1.2)π‘ . 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 π = 50(0.8)π‘ and graph (IV) is π = 50(0.6)π‘ . 27. We look for an equation of the form π¦ = π¦0 ππ₯ since the graph looks exponential. The points (0, 3) and (2, 12) are on the graph, so 3 = π¦0 π0 = π¦0 and
12 = π¦0 β π2 = 3 β π2 ,
giving
π = Β±2.
π₯
Since π > 0, our equation is π¦ = 3(2 ). 28. We look for an equation of the form π¦ = π¦0 ππ₯ since the graph looks exponential. The points (0, 18) and (2, 8) are on the graph, so 18 = π¦0 π0 = π¦0 β
and 2
2
8 = π¦0 β π = 18 β π ,
giving
π¦ = 18
( )π₯ 2 . 3
Since π > 0, our equation is
π=Β±
4 . 9
29. We look for an equation of the form π¦ = π¦0 ππ₯ since the graph looks exponential. The points (1, 6) and (2, 18) are on the graph, so 6 = π¦0 π1 and 18 = π¦0 π2 18 = 3, and so 6 = π¦0 π = π¦0 β 3; thus, π¦0 = 2. Hence π¦ = 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 π¦ = β2. Therefore we are looking for an equation of the form π¦ = πππ₯ β 2. Since at π₯ = 0 we have π¦ = 8 = π β 2, giving π = 10. The point (1, 4) is on the graph, so 4 = 10π1 β 2, giving π = 106 = 35 . Therefore, ( )π₯ 3 β 2. π¦ = 10 5 π¦ π2
Therefore π = π¦0 π = 0
31. We look for an equation of the form π¦ = π¦0 ππ₯ since the graph looks exponential. The points (β1, 8) and (1, 2) are on the graph, so 8 = π¦0 πβ1 and 2 = π¦0 π1 Therefore
π¦ πβ1 8 1 = 0 = 2 , giving π = 12 , and so 2 = π¦0 π1 = π¦0 β 12 , so π¦0 = 4. 2 ( )π¦0 π π
Hence π¦ = 4
1 2
π₯
.
32. The diο¬erence, π·, between the horizontal asymptote and the graph appears to decrease exponentially, so we look for an equation of the form π· = π·0 ππ₯ where π·0 = 4 = diο¬erence when π₯ = 0. Since π· = 4 β π¦, we have 4 β π¦ = 4ππ₯ or π¦ = 4 β 4ππ₯ = 4(1 β ππ₯ ) The point (1, 2) is on the graph, so 2 = 4(1 β π1 ), giving π = 12 . Therefore π¦ = 4(1 β ( 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 π» is a decreasing function of π that might be leveling oο¬ to an asymptote at π» = 0. These are features of an exponential decay function, but their presence does not show that π» is an exponential function of π . We can do a more precise check by dividing each value of π» by the previous yearβs π».
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 π» were an exponential function of π , the ratios would be approximately constant. Since they are not approximately constant, we see that an exponential model is a poor choice. π» 20 15 10 5 2010 2011 2012 2013 2014 2015
π
Figure 1.14 34. (a) See Figure 1.15. customers
time
Figure 1.15 (b) βThe rate at which new people try itβ 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 downβthe 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 diο¬erence 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 coο¬ee is all at the same temperature.) temperature
revenue
advertising
Figure 1.16
time
Figure 1.17
1.2 SOLUTIONS
19
36. (a) We have π0 = 1 million, and π = 0.02, so π = (1,000,000)(π0.02π‘ ). (b) π
1,000,000 π‘
37. If production continues to decay exponentially at a continuous rate of 9.1% per year, the production π (π‘) at time π‘ years after 2008 is π (π‘) = 84πβ0.091π‘ . In 2025, production is predicted to be π (17) = 84πβ0.091(17) = 17.882 million barrels per day. 38. (a) Let π represent the population of the world (in billions), and let π‘ represent the number of years since 2017. Then we have π = 7.41(1.011)π‘ . (b) According to this formula, the population of the world in the year 2025 (at π‘ = 8) will be π = 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 π = 14.82; we see on the graph that this occurs at approximately π‘ = 63.4. Under these assumptions, the doubling time of the worldβs population is about 63.4 years. π (billion people) 14.82 7.41 π‘ (years)
63.4
Figure 1.18
39. (a) Since the population was 2.7 million in 2010, and π‘ is measured since 2010 so π‘ = 0 in 2010, we have π0 = 2.7. Then π = 3.0 when π‘ = 8, so 3 = 2.7π8 ) ( 3 1β8 π= = 1.0133. 2.7 Thus,
π = 2.7(1.0133)π‘ .
(b) In 2000, we have π‘ = β10, so π = 2.7
((
3 2.7
)1β8 )β10
= 2.367 million.
40. Direct calculation reveals that each 1000 foot increase in altitude results in a longer takeoο¬ roll by a factor of about 1.096. Since the value of π when β = 0 (sea level) is π = 670, we are led to the formula π = 670(1.096)ββ1000 , where π is the takeoο¬ roll, in feet, and β is the airportβs elevation, in feet.
20
Chapter One /SOLUTIONS Alternatively, we can write
π = π0 πβ ,
where π0 is the sea level value of π, π0 = 670. In addition, when β = 1000, π = 734, so 734 = 670π1000 . Solving for π gives π= so
(
734 670
)1β1000
= 1.00009124,
π = 670(1.00009124)β .
41. Since we are told that the rate of decay is continuous, we use the function π(π‘) = π0 πππ‘ to model the decay, where π(π‘) is the amount of strontium-90 which remains at time π‘, and π0 is the original amount. Then π(π‘) = π0 πβ0.0247π‘ . So after 100 years, and
π(100) = π0 πβ0.0247β 100 π(100) = πβ2.47 β 0.0846 π0
so about 8.46% of the strontium-90 remains. 42. (a) Since π¦ 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 β 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 2π (π‘) = 6πππ‘ and π(π‘) = ππ2ππ‘ , we cannot ο¬nd a value of π that makes these functions equal. (b) Since (π (π‘))2 = (3πππ‘ )2 = 9π2ππ‘ , we can arrange that π(π‘) = (π (π‘))2 if ππ2ππ‘ = 9π2ππ‘ π = 9.
44. The doubling time π‘ depends only on the growth rate; it is the solution to 2 = (1.02)π‘ , since 1.02π‘ represents the factor by which the population has grown after time π‘. Trial and error shows that (1.02)35 β 1.9999 and (1.02)36 β 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 438β2 = 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 π(π‘) = π0 ππ‘ , where π is the annual growth factor. We have 438 = 219π12 , so 2 = π12 and π = 21β12 = 1.05946. Thus, π(π‘) = 219(1.05946)π‘ . (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 β 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 π‘ = 8.3. This second doubling has taken 8.3 β 6.0 = 2.3 years, the same amount of time as the ο¬rst doubling. Further comparison of any two populations on this graph that diο¬er 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 π = π0 ππ‘ doubles from time π‘ to time π‘+π. We now have π0 ππ‘+π = 2π0 ππ‘ , so π0 ππ‘ ππ = 2π0 ππ‘ . Thus, canceling π0 and ππ‘ , π must be the number such that ππ = 2, no matter what π‘ is. 47. (a) After 50 years, the amount of money is
π = 2π0 .
After 100 years, the amount of money is π = 2(2π0 ) = 4π0 . After 150 years, the amount of money is π = 2(4π0 ) = 8π0 . (b) The amount of money in the account doubles every 50 years. Thus in π‘ years, the balance doubles π‘β50 times, so π = π0 2π‘β50 . 48. (a) Since 162.5 = 325β2, there are 162.5 mg remaining after π» hours. Since 81.25 = 162.5β2, there are 81.25 mg remaining π» hours after there were 162.5 mg, so 2π» hours after there were 325 mg. Since 40.625 = 81.25β2, there are 41.625 mg remaining π» hours after there were 81.25 mg, so 3π» hours after there were 325 mg. (b) Each additional π» hours, the quantity is halved. Thus in π‘ hours, the quantity was halved π‘βπ» times, so π΄ = 325
( )π‘βπ» 1 . 2
49. (a) The quantity of radium decays exponentially, so we know π = π0 ππ‘ . When π‘ = 1620, we have π = π0 β2 so π0 = π0 π1620 . 2 Thus, canceling π0 , we have 1 2 ( )1β1620 1 π= = 0.999572 2
π1620 =
Thus the formula is π = π0 (0.999572)π‘ . (b) After 500 years, Fraction remaining =
1 β π0 (0.999572)500 = 0.80731. π0
so 80.731% is left. 50. Let π0 be the initial quantity absorbed in 1960. Then the quantity, π, of strontium-90 left after π‘ years is π = π0
( )π‘β29 1 . 2
Since 2010 β 1960 = 50 years, in 2010 Fraction remaining =
( )50β29 ( )50β29 1 1 1 β π0 = = 0.30268 = 30.268%. π0 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 ο¬nd π‘ such that π (π‘) = 5. We have 10(1β2)π‘β30 = 5 (1β2)π‘β30 = 1β2 π‘ =1 30 π‘ = 30, so the half-life is 30 years. To ο¬nd the continuous rate of decay, observe that π (π‘) = 10(1β2)π‘β30 = 10(πln(1β2) )π‘β30 = 10ππ‘ ln(1β2)β30 = 10πβ0.02310π‘ , so the continuous decay rate is 2.31% per year. 52. (a) The 1.109 represents the number of food parcels, in millions, when π‘ = 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 π0.12π‘ = (π0.12 )π‘ = 1.127π‘ , we see that the annual growth factor is 1.127. Thus, the annual growth rate is 1.127β1 = 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 oο¬ to π. (a) The value of π represents the value at which the concentration levels oο¬. (b) We see π is positive. (c) At π‘ = 0, we have π (0) = π β πππβ 0 = π β π. Since the graph goes through the origin, π (0) = 0. Thus π β π = 0 so π = π. (d) Since the concentration of π levels oο¬ to π and π (π‘) = π β ππππ‘ , the term ππππ‘ must decay to zero. To make the term ππππ‘ decay to zero, π must be negative. 54. (a) The function π appears to be exponential because ratios of successive output values of π are approximately equal for equally spaced π‘-values; that is 36.4 28.3 22.1 46.7 = = = β 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 πC, we can approximate by π = π (π‘) = 60(0.78)π‘ . (b) We want to solve for π‘ at which there is 30 πC (half the original 60) remaining: 30 = π (π‘) 30 = 60(0.78)π‘ 1 = 0.78π‘ 2 ln(1β2) = π‘ ln(0.78) ln(1β2) = 2.790. π‘= 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 π (π‘) = 60(0.78)π‘ = 60(πln(0.78) )π‘ = 60ππ‘ ln(0.78) = 60πβ0.248π‘ , 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 π = π (β), then π (0) = 760. This means π (β) has the form π (β) = 760 β πβ . We are also given that π (5.6) = 341, so 760 β π5.6 = 341 341 π5.6 = 760 ) ( 341 1β5.6 π= = 0.86666. 760
1.2 SOLUTIONS Therefore,
23
π = π (β) = 760(0.867)β .
(b) From part (a), we have π = 0.86666 = 1 + π, which means that π = 0.86666 β 1 = β0.13334. Therefore, the atmospheric pressure decreases by about 13.334% for each 1 km increase in elevation. (c) To ο¬nd the elevation where atmospheric pressure is 100 torr, we set π (β) = 100 and solve: π (β) = 100 760(0.86666)β = 100 100 0.86666β = 760 ) ( 100 β ln(0.86666) = ln 760 ln(100β760) β= = 14.172 km. ln(0.86666) 56. (a) Since the annual growth factor from 2012 to 2013 was 1 + (58.95β100) = 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 + (β0.0084) = 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 β 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 β 0.0397 = 0.9603 and 2.5941(1 β 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 ο¬gure 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 eο¬ect which makes the change more than 40%.
1.2 SOLUTIONS
25
61. (a) Since the π¦-intercept of each graph is above the π₯-axis, we know that π, π, and π must all be positive. (b) Since the graph of π¦ = πππ₯ is increasing and goes through (1, 1), the π¦-intercept, π, must be less than 1. Since the π¦-intercept is positive, we know that 0 < π < 1. Since π¦ = ππ π₯ and π¦ = ππ π₯ are both decreasing, both π and π must be between 0 and 1. (c) The graphs of π¦ = ππ π₯ and π¦ = ππ π₯ have the same π¦-intercepts, therefore we have π = π. (d) Since the point (1, 1) lies on the graph of π¦ = πππ₯ , we know that 1 = ππ1 . Therefore, π and π are reciprocals of each other. Similarly, π and π 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 π¦ = πβ0.25π₯ is decreasing but its graph is concave up. 64. The graph of π¦ = 2π₯ is a straight line and is neither concave up or concave down. 65. The last two points are not on the graph of ππ₯ . Points of the graph of this function have the form (π₯, ππ₯ ). The values π₯ = 2 and π₯ = 3 correspond to the points (2, π2 ) and (3, π3 ). 66. The functions π¦ = πβπ‘ and π¦ = (0.9)π‘ , for example, are both decreasing but have a vertical intercept of 1. To get a vertical intercept of π we must get this value when evaluating at π‘ = 0. Hence, two possible functions are π¦ = ππβπ‘ and π¦ = π(0.9)π‘ . 67. One possible answer is π = 2.2(0.97)π‘ . 68. One possible answer is π (π₯) = 2(1.1)π₯ . 69. One possibility is π¦ = πβπ₯ β 5. 70. Any exponential function of the form π¦ = ππ₯ , where 1 < π < π works. A possible example is π¦ = 2π₯ . 71. True. Using algebra and rules of exponents, we can rewrite π (π₯) so that it has the form π0 πππ₯ : π (π₯) = π2π₯ β(2π5π₯ ) 1 = π2π₯β5π₯ 2 1 β3π₯ = π . 2
72. False. The π¦-intercept is π¦ = 2 + 3πβ0 = 5. 73. True, since, as π‘ β β, we know πβ4π‘ β 0, so π¦ = 5 β 3πβ4π‘ β 5. 74. False. Suppose π¦ = 5π₯ . Then increasing π₯ by 1 increases π¦ by a factor of 5. However increasing π₯ by 2 increases π¦ by a factor of 25, not 10, since π¦ = 5π₯+2 = 5π₯ β 52 = 25 β 5π₯ . (Other examples are possible.) 75. True. Suppose π¦ = π΄ππ₯ and we start at the point (π₯1 , π¦1 ), so π¦1 = π΄ππ₯1 . Then increasing π₯1 by 1 gives π₯1 + 1, so the new π¦-value, π¦2 , is given by π¦2 = π΄ππ₯1 +1 = π΄ππ₯1 π = (π΄ππ₯1 )π, so π¦2 = ππ¦1 . Thus, π¦ has increased by a factor of π, so π = 3, and the function is π¦ = π΄3π₯ . However, if π₯1 is increased by 2, giving π₯1 + 2, then the new π¦-value, π¦3 , is given by π¦3 = π΄3π₯1 +2 = π΄3π₯1 32 = 9π΄3π₯1 = 9π¦1 . Thus, π¦ has increased by a factor of 9. 76. True. For example, π (π₯) = (0.5)π₯ is an exponential function which decreases. (Other examples are possible.) 77. True. If π > 1, then πππ₯ β 0 as π₯ β ββ. If 0 < π < 1, then πππ₯ β 0 as π₯ β β. In either case, the function π¦ = π + πππ₯ has π¦ = π as the horizontal asymptote. 78. True, since πβππ‘ β 0 as π‘ β β, so π¦ β 20 as π‘ β β.
Chapter One /SOLUTIONS
26
Solutions for Section 1.3 EXERCISES 1.
π¦
(a)
π¦
(b)
4
4
β2
2
π₯
π¦
π₯
β2
β2
π₯
π¦
(c)
2
π₯
β2
β4 π¦
4
π₯
β2
4
2
β4
π₯
π¦
(f)
4
2
2
β4 π¦
(e)
π₯
4
β2
β4
2
β4
4
2
β4
π₯
π¦
(b) 4
β2
2
β4 π¦
(d)
4
β2
β4
π₯
π¦
(f)
4
2
2
β4 π¦
(e)
β2
(a)
2
β2
π₯
β4
4
2.
4
β2
β4 (d)
π¦
(c)
π₯
β2
2
β4
π₯
1.3 SOLUTIONS 3.
π¦
(a)
π¦
(b) 4
β2
4
2
π₯
2
π₯
β2
2
β4 π¦
(e)
π¦
(f)
4
2
π₯
4
β2
β4
π₯
β4 π¦
4
β2
4
β2
β4 (d)
π¦
(c)
2
π₯
β2
β4
β4
4. This graph is the graph of π(π‘) shifted upward by two units. See Figure 1.22. 4 π(π‘)
β4
4
6
π‘
β4
Figure 1.22 5. This graph is the graph of π(π‘) shifted to the right by one unit. See Figure 1.23. π¦ 4
π(π‘) β4
4
β4
Figure 1.23
2
6
π‘
π₯
27
28
Chapter One /SOLUTIONS 6. This graph is the graph of π(π‘) shifted to the left by 1.5 units. See Figure 1.24. 4
π(π‘)
β4
4
π‘
6
β4
Figure 1.24 7. This graph is the graph of π(π‘) shifted to the right by 0.5 units and downward by 2.5 units. See Figure 1.25. 4
β4
π‘
6 π€(π‘) β4
Figure 1.25 8. Figure 1.26 shows the appropriate graphs. Note that asymptotes are shown as dashed lines and π₯- or π¦-intercepts are shown as ο¬lled circles. π¦
(a)
π¦
(b)
5
4 π¦=3
2
2
β5 β3
2
5 π¦
(c)
β5 β3
π₯
2
π₯
β2 π¦
(d)
5
5
5 π¦=4 2
2
1 β10
β6
β1
2
π₯ β5
Figure 1.26 9. (a) π (π(1)) = π (1 + 1) = π (2) = 22 = 4 (b) π(π (1)) = π(12 ) = π(1) = 1 + 1 = 2 (c) π (π(π₯)) = π (π₯ + 1) = (π₯ + 1)2 (d) π(π (π₯)) = π(π₯2 ) = π₯2 + 1 (e) π (π‘)π(π‘) = π‘2 (π‘ + 1)
β1
2
5
π₯
1.3 SOLUTIONS β β 2 10. (a) π (π(1)) = π (1 = 5 β ) = π (1) = β 1 + 4 β 2 (b) π(π (1)) = π( 1 + 4) β = π( 5) = ( 5) = 5 2 2 (c) π (π(π₯)) = π (π₯ β ) = π₯ +β4 (d) π(π (π₯)) = π(β π₯ + 4) = ( βπ₯ + 4)2 = π₯ + 4 (e) π (π‘)π(π‘) = ( π‘ + 4)π‘2 = π‘2 π‘ + 4 11. (a) π (π(1)) = π (12 ) = π (1) = π1 = π (b) π(π (1)) = π(π1 ) = π(π) = π2 2 (c) π (π(π₯)) = π (π₯2 ) = ππ₯ (d) π(π (π₯)) = π(ππ₯ ) = (ππ₯ )2 = π2π₯ (e) π (π‘)π(π‘) = ππ‘ π‘2 12. (a) π (π(1)) = π (3 β 1 + 4) = π (7) =
1 7
(b) π(π (1)) = π(1β1) = π(1) = 7 1 (c) π (π(π₯)) = π (3π₯ + 4) = 3π₯ ( )+ 4 ( ) 3 1 1 =3 +4= +4 (d) π(π (π₯)) = π π₯ π₯ π₯ 1 4 (e) π (π‘)π(π‘) = (3π‘ + 4) = 3 + π‘ π‘ 13. We have, for π₯ > 0 π (π(π₯)) β π(π (π₯)) = 14. We have,
15. We have,
(β )2 β π₯ β π₯2 = π₯ β π₯ = 0.
π (π(π₯)) β π(π (π₯)) = 3(2π₯) β 2(3π₯) = 0.
π (π(π₯)) β π(π (π₯)) = 3(2π₯) + 1 β 2(3π₯ + 1) = 6π₯ + 1 β 6π₯ β 2 = β1.
16. We have,
2
2
π (π(π₯)) β π(π (π₯)) = (ππ₯ )2 β ππ₯ = π2π₯ β ππ₯ .
This cannot be simpliο¬ed. 17. (a) π (π‘ + 1) = (π‘ + 1)2 + 1 = π‘2 + 2π‘ + 1 + 1 = π‘2 + 2π‘ + 2. (b) π (π‘2 + 1) = (π‘2 + 1)2 + 1 = π‘4 + 2π‘2 + 1 + 1 = π‘4 + 2π‘2 + 2. (c) π (2) = 22 + 1 = 5. (d) 2π (π‘) = 2(π‘2 + 1) = 2π‘2 + 2. ( )2 (e) (π (π‘))2 + 1 = π‘2 + 1 + 1 = π‘4 + 2π‘2 + 1 + 1 = π‘4 + 2π‘2 + 2. 18. (a) π(2 + β) = (2 + β)2 + 2(2 + β) + 3 = 4 + 4β + β2 + 4 + 2β + 3 = β2 + 6β + 11. (b) π(2) = 22 + 2(2) + 3 = 4 + 4 + 3 = 11, which agrees with what we get by substituting β = 0 into (a). (c) π(2 + β) β π(2) = (β2 + 6β + 11) β (11) = β2 + 6β. 19. π(π§ + 1) β π(π§) = (π§ + 1)2 β π§2 = 2π§ + 1. 20. π(π§ + β) β π(π§) = (π§ + β)2 β π§2 = 2π§β + β2 . 21. π(π§) β π(π§ β β) = π§2 β (π§ β β)2 = 2π§β β β2 . 22. π(π§ + β) β π(π§ β β) = (π§ + β)2 β (π§ β β)2 = π§2 + 2βπ§ + β2 β (π§2 β 2βπ§ + β2 ) = 4βπ§. 23.
π (βπ₯) = (βπ₯)6 + (βπ₯)3 + 1 = π₯6 β π₯3 + 1. Since π (βπ₯) β π (π₯) and π (βπ₯) β βπ (π₯), this function is neither even nor odd.
24.
π (βπ₯) = (βπ₯)3 + (βπ₯)2 + (βπ₯) = βπ₯3 + π₯2 β π₯. Since π (βπ₯) β π (π₯) and π (βπ₯) β βπ (π₯), this function is neither even nor odd.
25. Since we see π is even
π (βπ₯) = (βπ₯)4 β (βπ₯)2 + 3 = π₯4 β π₯2 + 3 = π (π₯),
29
30
Chapter One /SOLUTIONS
26. Since
π (βπ₯) = (βπ₯)3 + 1 = βπ₯3 + 1,
we see π (βπ₯) β π (π₯) and π (βπ₯) β βπ (π₯), so π is neither even nor odd 27. Since
π (βπ₯) = 2(βπ₯) = β2π₯ = βπ (π₯),
we see π is odd. 28. Since
2
2
π (βπ₯) = π(βπ₯) β1 = ππ₯ β1 = π (π₯),
we see π is even. 29. Since
π (βπ₯) = (βπ₯)((βπ₯)2 β 1) = βπ₯(π₯2 β 1) = βπ (π₯),
we see π is odd 30. Since
π (βπ₯) = πβπ₯ + π₯,
we see π (βπ₯) β π (π₯) and π (βπ₯) β βπ (π₯), so π 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 π (π₯) = π₯2 + 3π₯ + 2 two times, π is not invertible. See Figure 1.27. π¦ 4
π (π₯) = π₯2 + 3π₯ + 2
π¦ = 2.5
3 2
π₯
β3
Figure 1.27 34. Since a horizontal line cuts the graph of π (π₯) = π₯3 β 5π₯ + 10 three times, π is not invertible. See Figure 1.28. π¦
π (π₯) = π₯3 β 5π₯ + 10
10 π¦=8 π₯ -2
2 Figure 1.28
1.3 SOLUTIONS
31
35. Since any horizontal line cuts the graph once, π is invertible. See Figure 1.29. π¦ π (π₯) = π₯3 + 5π₯ + 10
40
π¦ = 30 20 -2
2 π₯ π¦ = β19
Figure 1.29 36. (a) π (25) is π corresponding to π = 25, or, in other words, the number of items sold when the price is 25. (b) π β1 (30) is π corresponding to π = 30, or the price at which 30 units will be sold. 37. (a) π (10,000) represents the value of πΆ corresponding to π΄ = 10,000, or in other words the cost of building a 10,000 square-foot store. (b) π β1 (20,000) represents the value of π΄ corresponding to πΆ = 20,000, or the area in square feet of a store which would cost $20,000 to build. 38. π β1 (75) is the length of the column of mercury in the thermometer when the temperature is 75β¦ F. 39. (a) The equation is π¦ = 2π₯2 + 1. Note that its graph is narrower than the graph of π¦ = π₯2 which appears in gray. See Figure 1.30. 8
π¦ = 2π₯2 + 1
6 4
π¦ = π₯2
2
Figure 1.30
8 7 6 5 4 3 2 1
π¦ = 2(π₯2 + 1)
π¦ = π₯2
Figure 1.31
(b) π¦ = 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 ο¬rst.
PROBLEMS 40. Since π = π β ππβππ‘ , the graph of π is the reο¬ection of π¦ about the π‘-axis moved up by π units. 41. This looks like a shift of the graph π¦ = βπ₯2 . The graph of π¦ = βπ₯2 is shifted to the left 1 unit and up 3 units, so a possible formula is π¦ = β(π₯ + 1)2 + 3. The graph of π¦ = βπ₯2 is the graph of π¦ = π₯2 reο¬ected in the π₯-axis. 42. This looks like a shift of the graph π¦ = π₯3 . The graph is shifted to the right 2 units and down 1 unit, so a possible formula is π¦ = (π₯ β 2)3 β 1. 43. We have π£(10) = 65 but the graph of π’ only enables us to evaluate π’(π₯) for 0 β€ π₯ β€ 50. There is not enough information to evaluate π’(π£(10)).
32
Chapter One /SOLUTIONS
44. We have approximately π£(40) = 15 and π’(15) = 18 so π’(π£(40)) = 18. 45. We have approximately π’(10) = 13 and π£(13) = 60 so π£(π’(10)) = 60. 46. We have π’(40) = 60 but the graph of π£ only enables us to evaluate π£(π₯) for 0 β€ π₯ β€ 50. There is not enough information to evaluate π£(π’(40)). 47. π (π(1)) = π (2) β 0.4. 48. π(π (2)) β π(0.4) β 1.1. 49. π (π (1)) β π (β0.4) β β0.9. 50. Computing π (π(π₯)) as in Problem 47, we get Table 1.4. From it we graph π (π(π₯)) in Figure 1.32. Table 1.4 π₯
π(π₯)
π (π(π₯))
β3
0.6
β0.5
β2.5
β1.1
β1.3
β2
β1.9
β1.2
β1.5
β1.9
β1.2 β1.3
β1
β1.4
β0.5
β0.5
β1
0
0.5
β0.6
0.5
1.4
β0.2
3
π (π(π₯)) π₯ 3
β3
1
2
0.4
1.5
2.2
0.5
2
1.6
0
2.5
0.1
β0.7
β3
3
β2.5
0.1
Figure 1.32
51. Using the same way to compute π(π (π₯)) as in Problem 48, we get Table 1.5. Then we can plot the graph of π(π (π₯)) in Figure 1.33. Table 1.5 π₯
π (π₯)
π(π (π₯))
β3
3
β2.6
β2.5
0.1
0.8
β2
β1
β1.4
β1.5
β1.3
β1.8
β1
β1.2
β1.7
β0.5
β1
β1.4
0
β0.8
β1
0.5
β0.6
β0.6
1
β0.4
β0.3
1.5
β0.1
0.3
3
β3
π(π (π₯))
3
2
0.3
1.1
2.5
0.9
2
β3
3
1.6
2.2
Figure 1.33
π₯
52. Using the same way to compute π (π (π₯)) as in Problem 49, we get Table 1.6. Then we can plot the graph of π (π (π₯)) in Figure 1.34.
1.3 SOLUTIONS
33
Table 1.6 π₯
π (π₯)
π (π (π₯))
β3
3
1.6
β2.5
0.1
β0.7
β2
β1
β1.2
β1.5
β1.3
β1.3
β1
β1.2
β1.3
β0.5
β1
β1.2
0
β0.8
β1.1
0.5
β0.6
β1
3 π (π (π₯))
β3
3
1
β0.4
β0.9
1.5
β0.1
β0.8
2
0.3
β0.6
2.5
0.9
β0.4
β3
3
1.6
0
Figure 1.34
53. π (π₯) = π₯3 ,
π₯
π(π₯) = π₯ + 1.
54. π (π₯) = π₯ + 1, π(π₯) = π₯3 . β 55. π (π₯) = π₯, π(π₯) = π₯2 + 4 56. π (π₯) = ππ₯ ,
π(π₯) = 2π₯
57. The tree has π΅ = π¦ β 1 branches on average and each branch has π = 2π΅ 2 β π΅ = 2(π¦ β 1)2 β (π¦ β 1) leaves on average. Therefore Average number of leaves = π΅π = (π¦ β 1)(2(π¦ β 1)2 β (π¦ β 1)) = 2(π¦ β 1)3 β (π¦ β 1)2 . 58. The volume, π , of the balloon is π = 43 ππ3 . When π‘ = 3, the radius is 10 cm. The volume is then π =
4 4000π π(103 ) = cm3 . 3 3
59. Since π is even, we know that π (π₯) = π₯. Since π is odd, we know that π(π₯) = βπ₯. Since β(π₯) = π(π (π₯) and π(π₯) is odd, we know that β(π₯) = βπ (π₯), and since π (π₯) = π₯, we know that β(π₯) = βπ₯. Using this, we ο¬ll in Table 1.7. Table 1.7 π₯
π (π₯)
π(π₯)
β(π₯)
β3
0
0
0
β2
2
2
β2
β1
2
2
β2
0
0
0
0
1
2
β2
β2
2
2
β2
β2
3
0
0
0
π₯
3
β7
19
4
178
2
1
π β1 (π₯)
1
2
3
4
5
6
7
60. Values of π β1 are as follows
The domain of π β1 is the set consisting of the integers {3, β7, 19, 4, 178, 2, 1}.
34
Chapter One /SOLUTIONS
61. (a) We ο¬nd π β1 (2) by ο¬nding the π₯ value corresponding to π (π₯) = 2. Looking at the graph, we see that π β1 (2) = β1. (b) We construct the graph of π β1 (π₯) by reο¬ecting the graph of π (π₯) over the line π¦ = π₯. The graphs of π β1 (π₯) and π (π₯) are shown together in Figure 1.35. π¦ 4 π (π₯) β4
6
π₯
π β1 (π₯) β4
Figure 1.35
62. π is an increasing function since the amount of fuel used increases as ο¬ight time increases. Therefore π is invertible. 63. Not invertible. Given a certain number of customers, say π (π‘) = 1500, there could be many times, π‘, during the day at which that many people were in the store. So we donβt 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 and π, with π (π) = π (π) = 0. Hence we donβt know what to choose for π β1 (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 π‘ minutes after inο¬ation began is: π(π (π‘)) ft3 . 72. The volume of the balloon if its radius were twice as big is: π(2π) ft3 . 73. The time elapsed is: π β1 (30) min. 74. The time elapsed is: π β1 (π β1 (10,000)) min. 75. (a) The function π tells us πΆ in terms of π. To get its inverse, we want π in terms of πΆ, which we ο¬nd by solving for π: πΆ = 100 + 2π, πΆ β 100 = 2π, πΆ β 100 π= = π β1 (πΆ). 2 (b) The inverse function tells us the number of articles that can be produced for a given cost. 76. (a) Yes, π is invertible, since π is increasing everywhere. (b) The number π β1 (400) is the year in which 400 million motor vehicles were registered in the world. From the picture, we see that π β1 (400) is around 1979. (c) Since the graph of π β1 is the reο¬ection of the graph of π over the line π¦ = π₯, we get Figure 1.36.
1.3 SOLUTIONS
35
(year) β10 β05 β00 β95 β90 β85 β80 β75 β70 β65
200
400
600
800
1000
(millions)
Figure 1.36: Graph of π β1
77. (a) The graph shows that π (15) is approximately 48. So, the place to ο¬nd ο¬nd 15 million-year-old rock is about 48 meters below the Atlantic sea ο¬oor. (b) Since π is increasing (not decreasing, since the depth axis is reversed!), π is invertible. To conο¬rm, notice that the graph of π is cut by a horizontal line at most once. (c) Look at where the horizontal line through 120 intersects the graph of π and read downward: π β1 (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 π so that time and depth are increasing from left to right and bottom to top. Points (π‘, π) on the graph of π correspond to points (π, π‘) on the graph of π β1 . We can graph π β1 by taking points from the original graph of π , reversing their coordinates, and connecting them. This amounts to interchanging the π‘ and π axes, thereby reο¬ecting the graph of π about the line bisecting the 90β¦ angle at the origin. Figure 1.37 is the graph of π β1 . (Note that we cannot ο¬nd the graph of π β1 by ο¬ipping the graph of π about the line π‘ = π in because π‘ and π have diο¬erent scales in this instance.)
π β1
30
100
Time
Depth π (standardized)
10
20 10
Time
30 20
Figure 1.37: Graph of π , reο¬ected to give that of π
Depth
100
β1
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₯) β step(βπ₯) = 1 β 0 = 1, and for negative π₯ we have step(π₯) β step(βπ₯) = 0 β 1 = β1. The formula describes the sign function. (c) For positive π₯, we have π₯ step(π₯) β π₯ step(βπ₯) = π₯ β 0 = π₯, and for negative π₯ we have π₯ step(π₯) β π₯ step(βπ₯) = 0 β π₯ = βπ₯. The formula describes the absolute value function.
Strengthen Your Understanding 79. The graph of π (π₯) = β(π₯ + 1)3 is the graph of π(π₯) = βπ₯3 shifted left by 1 unit. 80. The graphs of inverse functions are symmetric with respect to the line π¦ = π₯. Graphing these two functions for π₯ > 0, we see that they are both concave up on the ο¬rst quadrant, and hence not symmetric with respect to the line π¦ = π₯. 81. Since π (π(π₯)) = 3(β3π₯ β 5) + 5 = β9π₯ β 10, we see that π and π 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₯
π (π (π₯)) = π (ππ₯ ) = ππ = (ππ )π₯ β (15.154)π₯ β π₯. 83. While π¦ = 1βπ₯ is sometimes referred to as the multiplicative inverse of π₯, the inverse of π is π β1 (π₯) = π₯. 84. One possible answer is π(π₯) = 3 + π₯. (There are many answers.) 85. One possibility is π (π₯) = π₯2 + 2. 86. Let π (π₯) = 3π₯, then π β1 (π₯) = π₯β3. Then for π₯ > 0, we have π (π₯) > π β1 (π₯). 87. We have
π(π₯) = π (π₯ + 2)
because the graph of π is obtained by moving the graph of π to the left by 2 units. We also have π(π₯) = π (π₯) + 3 because the graph of π is obtained by moving the graph of π up by 3 units. Thus, we have π (π₯ + 2) = π (π₯) + 3. The graph of π climbs 3 units whenever π₯ increases by 2. The simplest choice for π is a linear function of slope 3β2, for example π (π₯) = 1.5π₯, so π(π₯) = 1.5π₯ + 3. 88. True. Using properties of exponents we see that:
( )π₯ π₯ π (π(π₯)) = π (3π₯ ) = 23 = 23 = 8π₯ .
So, we see π (π(π₯)) = 8π₯ is exponential. Similarly, we can check π(π (π₯)) = 9π₯ is exponential. In general, the composition of two exponential functions of form π¦ = πΆππ₯ is exponential. 89. True. The graph of π¦ = 10π₯ is moved horizontally by β units if we replace π₯ by π₯ββ for some number β. Writing 100 = 102 , we have π (π₯) = 100(10π₯ ) = 102 β 10π₯ = 10π₯+2 . The graph of π (π₯) = 10π₯+2 is the graph of π(π₯) = 10π₯ shifted two units to the left. 90. True. If π is increasing then its reο¬ection about the line π¦ = π₯ is also increasing. An example is shown in Figure 1.38. The statement is true. π¦
π₯=π¦
4 π (π₯)
β4
6
π₯
π β1 (π₯) β4
Figure 1.38 91. True. If π (π₯) is even, we have π (π₯) = π (βπ₯) for all π₯. For example, π (β2) = π (2). This means that the graph of π (π₯) intersects the horizontal line π¦ = π (2) at two points, π₯ = 2 and π₯ = β2. Thus, π has no inverse function. 92. False. For example, π (π₯) = π₯ and π(π₯) = π₯3 are both odd. Their inverses are π β1 (π₯) = π₯ and π β1 (π₯) = π₯1β3 . 2
93. False. For π₯ < 0, as π₯ increases, π₯2 decreases, so πβπ₯ increases. 94. True. We have π(βπ₯) = π(π₯) since π is even, and therefore π (π(βπ₯)) = π (π(π₯)). 95. False. A counterexample is given by π (π₯) = π₯2 and π(π₯) = π₯ + 1. The function π (π(π₯)) = (π₯ + 1)2 is not even because π (π(1)) = 4 and π (π(β1)) = 0 β 4. 96. True. The constant function π (π₯) = 0 is the only function that is both even and odd. This follows, since if π is both even and odd, then, for all π₯, π (βπ₯) = π (π₯) (if π is even) and π (βπ₯) = βπ (π₯) (if π is odd). Thus, for all π₯, π (π₯) = βπ (π₯) i.e. π (π₯) = 0, for all π₯. So π (π₯) = 0 is both even and odd and is the only such function. 97. True. A linear function can be written as π¦ = π + ππ₯. Hence, writing π (π₯) = π + ππ₯ and π(π₯) = π + ππ₯ and using algebra, we see that: π (π(π₯)) = π (π + ππ₯) = π + π(π + ππ₯) = π + ππ + πππ₯. So, setting π = π + ππ and π = ππ, we see that π (π(π₯)) is of the form π + ππ₯. Similarly, we can check π(π (π₯)) is of this form.
1.4 SOLUTIONS
37
98. Let π (π₯) = π₯ and π(π₯) = β2π₯. Then π (π₯) + π(π₯) = βπ₯, which is decreasing. Note π is increasing since it has positive slope, and π is decreasing since it has negative slope. 99. This is impossible. If π < π, then π (π) < π (π), since π is increasing, and π(π) > π(π), since π is decreasing, so βπ(π) < βπ(π). Therefore, if π < π, then π (π) β π(π) < π (π) β π(π), which means that π (π₯) + π(π₯) is increasing. 100. Let π (π₯) = ππ₯ and let π(π₯) = πβ2π₯ . Note π is increasing since it is an exponential growth function, and π is decreasing since it is an exponential decay function. Then π (π₯)π(π₯) = πβπ₯ , which is decreasing. 101. This is impossible. As π₯ increases, π(π₯) decreases. As π(π₯) decreases, so does π (π(π₯)) because π 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 πln π₯ = π₯, we have πln(1β2) = 12 . 2. Using the identity 10log π₯ = π₯, we have
10log(π΄π΅) = π΄π΅
3. Using the identity πln π₯ = π₯, we have 5π΄2 . 4. Using the identity ln (ππ₯ ) = π₯, we have 2AB. 5. Using the rules for ln, we have ln
( ) 1 + ln π΄π΅ = ln 1 β ln π + ln π΄ + ln π΅ π = 0 β 1 + ln π΄ + ln π΅ = β1 + ln π΄ + ln π΅.
6. Using the rules for ln, we have 2π΄ + 3π ln π΅. 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 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(2β5) π₯= = β23.4. 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(4β7) π₯= β β1.1. log(5β3)
11. To solve for π₯, we ο¬rst divide both sides by 5 and then take the natural logarithm of both sides. 7 = π0.2π₯ 5 ln(7β5) = 0.2π₯ ln(7β5) β 1.68. π₯= 0.2 12.
ln(2π₯ ) = ln(ππ₯+1 ) π₯ ln 2 = (π₯ + 1) ln π π₯ ln 2 = π₯ + 1
0.693π₯ = π₯ + 1 1 π₯= β β3.26 0.693 β 1 13. To solve for π₯, we ο¬rst divide both sides by 600 and then take the natural logarithm of both sides. 50 = πβ0.4π₯ 600 ln(50β600) = β0.4π₯ ln(50β600) β 6.212. π₯= β0.4 14.
ln(2π3π₯ ) = ln(4π5π₯ ) ln 2 + ln(π3π₯ ) = ln 4 + ln(π5π₯ ) 0.693 + 3π₯ = 1.386 + 5π₯ π₯ = β0.347
15. Using the rules for ln, we get ln 7π₯+2 = ln π17π₯ (π₯ + 2) ln 7 = 17π₯ π₯(ln 7 β 17) = β2 ln 7 β2 ln 7 β 0.26. π₯= ln 7 β 17 16.
ln(10π₯+3 ) = ln(5π7βπ₯ ) (π₯ + 3) ln 10 = ln 5 + (7 β π₯) ln π 2.303(π₯ + 3) = 1.609 + (7 β π₯) 3.303π₯ = 1.609 + 7 β 2.303(3) π₯ = 0.515
1.4 SOLUTIONS
39
17. Using the rules for ln, we have 2π₯ β 1 = π₯2 2
π₯ β 2π₯ + 1 = 0 (π₯ β 1)2 = 0 π₯ = 1. 4π2π₯β3 = π + 5
18.
ln 4 + ln(π2π₯β3 ) = ln(π + 5) 1.3863 + 2π₯ β 3 = 2.0436 π₯ = 1.839. log π 19. π‘ = . log π ( ) log ππ log π β log π0 0 = . 20. π‘ = log π log π 21. Taking logs of both sides yields ππ‘ = Hence π‘=
log
(
π π0
ln ππ
0
π
.
=
log π β log π0 . π log π
( )π‘ π π = 0. π π0
π‘=
π = ππ‘, so π‘ = 24. ln π0
)
log π
Hence
π 23. π‘ = ln . π
π π0
)
π log π
22. Collecting similar terms yields
(
log
log
(
log
π0
)
π0
( ). π π
.
25. Since we want (1.5)π‘ = πππ‘ = (ππ )π‘ , so 1.5 = ππ , and π = ln 1.5 = 0.4055. Thus, π = 15π0.4055π‘ . Since 0.4055 is positive, this is exponential growth. 26. We want 1.7π‘ = πππ‘ so 1.7 = ππ and π = ln 1.7 = 0.5306. Thus π = 10π0.5306π‘ . 27. We want 0.9π‘ = πππ‘ so 0.9 = ππ and π = ln 0.9 = β0.1054. Thus π = 174πβ0.1054π‘ . 28. Since we want (0.55)π‘ = πππ‘ = (ππ )π‘ , so 0.55 = ππ , and π = ln 0.55 = β0.5978. Thus π = 4πβ0.5978π‘ . Since β0.5978 is negative, this represents exponential decay. 29. If π(π‘) = (1.04)π‘ , then, for πβ1 the inverse of π, we should have (1.04)π
β1 (π‘)
= π‘,
β1
π (π‘) log(1.04) = log π‘, log π‘ β 58.708 log π‘. πβ1 (π‘) = log(1.04) 30. Since π is increasing, π has an inverse. To ο¬nd the inverse of π (π‘) = 50π0.1π‘ , we replace π‘ with π β1 (π‘), and, since π (π β1 (π‘)) = π‘, we have β1 π‘ = 50π0.1π (π‘) .
40
Chapter One /SOLUTIONS We then solve for π β1 (π‘): π‘ = 50π0.1π
β1 (π‘)
β1 π‘ = π0.1π (π‘) 50 ( ) π‘ = 0.1π β1 (π‘) ln 50 ( ) ( ) 1 π‘ π‘ = 10 ln . ln π β1 (π‘) = 0.1 50 50
31. Using π (π β1 (π‘)) = π‘, we see
π (π β1 (π‘)) = 1 + ln π β1 (π‘) = π‘.
So ln π β1 (π‘) = π‘ β 1 π β1 (π‘) = ππ‘β1 .
PROBLEMS 32. Since π¦(0) = πΆπ0 = πΆ we have that πΆ = 2. Similarly, substituting π₯ = 1 gives π¦(1) = 2ππΌ so 2ππΌ = 1. Rearranging gives ππΌ = 1β2. Taking logarithms we get πΌ = ln(1β2) = β ln 2 = β0.693. Finally, π¦(2) = 2π2(β ln 2) = 2πβ2 ln 2 =
1 . 2
33. At the doubling time, π‘ = 10, we have π = 2π0 . Thus π0 π10π = 2π0 π10π = 2 10π = ln 2 1 ln 2 = 0.0693. π= 10 The function π = π0 π0.0693π‘ has doubling time equal to 10. 34. At the doubling time, π‘ = 0.4, the we have π = 2π0 . Thus π0 π0.4π = 2π0 π0.4π = 2 0.4π = ln 2 1 ln 2 = 1.733. π= 0.4 The function π = π0 π1.733π‘ has doubling time equal to 0.4. 35. Since ln π (π‘) = logπ π (π‘), we have Thus,
ππ (π‘) = πln π‘+2.3 = πln π‘ β π2.3 = π‘π2.3 . π (π‘) = ln(ππ (π‘) ) = ln(π‘π2.3 ).
Using the approximation 2.3 = ln 10 or π2.3 = 10, we have π (π‘) = ln(π‘π2.3 ) = ln(10π‘).
1.4 SOLUTIONS
41
36. We can solve for the growth rate π of the bacteria using the formula π = π0 πππ‘ : 1500 = 500ππ(2) ln(1500β500) π= . 2 Knowing the growth rate, we can ο¬nd the population π at time π‘ = 6: ln 3
π = 500π( 2 )6 β 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 π (π‘) = 282.2πππ‘ at time π‘ years after 2000. Using the 2018 population, which corresponds to π‘ = 18, we have 327.2 = 282.2π18π ln(327.2β282.2) π= = 0.0082198. 18 We want to ο¬nd the time π‘ in which 350 = 282.2π0.0082198π‘ ln(350β282.2) π‘= = 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 π = 282.2π0.0082198π‘ for π‘ = 20 to ο¬nd π = 332.6 million people. 39. The population has increased by a factor of 48,000,000β40,000,000 = 1.2 in 10 years. Thus we have the formula π = 40,000,000(1.2)π‘β10 , and π‘β10 gives the number of 10-year periods that have passed since 2005. In 2005, π‘β10 = 0, so we have π = 40,000,000. In 2015, π‘β10 = 1, so π = 40,000,000(1.2) = 48,000,000. In 2020, π‘β10 = 1.5, so π = 40,000,000(1.2)1.5 β 52,581,000. To ο¬nd the doubling time, solve 80,000,000 = 40,000,000(1.2)π‘β10 , to get π‘ = 38.02 years. 40. Let π (π‘) be oil consumption π‘ years after 2015. Since consumption is exponential, and π (0) = 11.986 million barrels per day, we have π (π‘) = 11.986πππ‘ . In 2018, when π‘ = 3, consumption was 13.525, so π (3) = 13.525 11.986π3π‘ = 13.525 ) ( 13.525 3π‘ = ln 11.986 π = 0.040267. Our model predicts Chinese oil consumption in 2025, when π‘ = 10, to be π (10) = 11.986π0.040267(10) = 17.929 million barrels per day. 41. If πΆ0 is the concentration of NO2 on the road, then the concentration π₯ meters from the road is πΆ = πΆ0 πβ0.0254π₯ . We want to ο¬nd the value of π₯ making πΆ = πΆ0 β2, that is, πΆ0 πβ0.0254π₯ =
πΆ0 . 2
42
Chapter One /SOLUTIONS Dividing by πΆ0 and then taking natural logs yields ( ) ( ) 1 = β0.6931, ln πβ0.0254π₯ = β0.0254π₯ = 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 π0 is the number of deaths per year without pollution, then the number of deaths per year, π, when the quantity of pollution is π₯ micrograms per cubic meter of air is π = π0 (1.0033)π₯ . (b) We want to ο¬nd the value of π₯ making π = 2π0 , that is, π0 (1.0033)π₯ = 2π0 . Dividing by π0 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 393,553β302,341 = 91,212 between 2012 to 2017. Thus the percent increase is 91,212β302,341 = 0.302 = 30.2%. Alternatively, we see that 393,553β30,2341 = 1.302, again showing an increase of 30.2%. (b) To ο¬nd π΄, we solve when π‘ = 0: π΄ππβ 0 = 302,341 π΄ β 1 = 302,341 π΄ = 302,341. Since π‘ is the number of years since 2012, we know that π‘ = 5 in 2017 and get: 393,553 = 302,341π5π . Solving for π, we get 393,553 = π5π 302,341 ( ) 393,553 ln = 5π 302,341 π = 0.052732. Substituting π‘ = 1, 2, 3, 4 into
302,341π(0.052732)π‘ ,
we ο¬nd 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 π‘ = β1. Therefore, If π is the number of E85-powered vehicles in 2011, we have π = 302,341π0.052732(β1) = 286,811.
1.4 SOLUTIONS
43
44. (a) Since the initial amount of caο¬eine is 100 mg and the exponential decay rate is β0.17, we have π΄ = 100πβ0.17π‘ . (b) See Figure 1.39. We estimate the half-life by estimating π‘ when the caο¬eine is reduced by half (so π΄ = 50); this occurs at approximately π‘ = 4 hours. π΄ (mg) 100
50
π‘ (hours)
4
Figure 1.39 (c) We want to ο¬nd the value of π‘ when π΄ = 50: 50 = 100πβ0.17π‘ 0.5 = πβ0.17π‘ ln 0.5 = β0.17π‘ π‘ = 4.077. The half-life of caο¬eine 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 πΆ = 100πππ‘ . We can evaluate π by using the value πΆ = 25 at π‘ = 10. 25 = 100π10π 0.25 = π10π ln(0.25) = 10π π = β0.139. An exponential model is given by
πΆ = 100πβ0.139π‘ .
Alternative solution. Using the half-life π = 5 years, we have πΆ = 100 β 2βπ‘βπ = 100 β 2βπ‘β5 . 46. (a) The initial dose is 10 mg. (b) Since 0.82 = 1 β 0.18, the decay rate is 0.18, so 18% leaves the body each hour. (c) When π‘ = 6, we have π΄ = 10(0.82)6 = 3.04. The amount in the body after 6 hours is 3.04 mg. (d) We want to ο¬nd the value of π‘ when π΄ = 1. Using logarithms: 1 = 10(0.82)π‘ 0.1 = (0.82)π‘ ln(0.1) = π‘ ln(0.82) π‘ = 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 π β¦ F, we have π = π0 (1.04)π β32 . (b) At 50β¦ F, we have
π1 = π0 (1.04)50β32 = π0 (1.04)18 .
β¦
And at 14 F, we have Thus
π2 = π0 (1.04)14β32 = π0 (1.04)β18 . π (1.04)β18 π2 = 0 = 1.04β36 = 0.244. π1 π0 (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 2π0 = π0 (1.04)π (1.04)π = 2 π ln 1.04 = ln 2 ln 2 = 17.7. π = ln 1.04 So an approximately 18β¦ F temperature rise doubles the amount of moisture that can be absorbed. 48. To ο¬nd a half-life, we want to ο¬nd at what π‘ value π = 12 π0 . Plugging this into the equation of the decay of plutonium-240, we have 1 = πβ0.00011π‘ 2 ln(1β2) π‘= β 6,301 years. β0.00011 The only diο¬erence in the case of plutonium-242 is that the constant β0.00011 in the exponent is now β0.0000018. Thus, following the same procedure, the solution for π‘ is π‘=
ln(1β2) β 385,081 years. β0.0000018
49. Given the doubling time of 5 hours, we can solve for the bacteriaβs growth rate; 2π0 = π0 ππ5 ln 2 π= . 5 So the growth of the bacteria population is given by: π = π0 πln(2)π‘β5 . We want to ο¬nd π‘ such that
3π0 = π0 πln(2)π‘β5 .
Therefore we divide both sides by π0 and apply ln. We get π‘=
5 ln(3) = 7.925 hours. ln(2)
50. (a) The pressure π at 6194 meters is given in terms of the pressure π0 at sea level to be π = π0 πβ0.00012β = π0 π(β0.00012)6194 = π0 πβ0.74328 β 0.4756π0
or about 47.6% of sea level pressure.
1.4 SOLUTIONS
45
(b) At β = 12,000 meters, we have π = π0 πβ0.00012β = π0 π(β0.00012)12,000 = π0 πβ1.44 β 0.2369π0
or about 23.7% of sea level pressure.
51. (a) π΅(π‘) = π΅0 π0.067π‘ (b) π (π‘) = π0 π0.033π‘ (c) If the initial price is $50, then
π΅(π‘) = 50π0.067π‘ π (π‘) = 50π0.033π‘ .
We want the value of π‘ such that
π΅(π‘) = 2π (π‘) 50π0.067π‘ = 2 β 50π0.033π‘ π0.067π‘ = π0.034π‘ = 2 π0.033π‘ ln 2 π‘= = 20.387 years . 0.034 Thus, when π‘ = 20.387 the price of the textbook was predicted to be double what it would have been had the price risen by inο¬ation only. This occurred in the year 2000.
52. (a) We assume π (π‘) = π΄πβππ‘ , where π΄ is the initial population, so π΄ = 100,000. When π‘ = 110, there were 3200 tigers, so 3200 = 100,000πβπβ 110 Solving for π gives 3200 = 0.032 πβπβ 110 = 100,000 1 π=β ln(0.032) = 0.0313 = 3.13% 110 so π (π‘) = 100,000πβ0.0313π‘ . (b) In 2000, the predicted number of tigers was π (100) = 100,000πβ0.0313(100) = 4372. In 2010, we know the number of tigers was 3200. The predicted percent reduction is 3200 β 4372 = β0.268 = β26.8%. 4372 Thus the actual decrease is larger than the predicted decrease. 53. The population of China, πΆ, in billions, is given by πΆ = 1.379(1.0041)π‘ where π‘ is time in years from 2017, and the population of India, πΌ, in billions, is given by πΌ = 1.282(1.0117)π‘ . The two populations will be equal when πΆ = πΌ, thus, we must solve the equation: 1.379(1.0041)π‘ = 1.282(1.0117)π‘ for π‘, which leads to
(1.0117)π‘ ( 1.0117 )π‘ 1.379 = . = 1.282 (1.0041)π‘ 1.0041
Taking logs on both sides, we get π‘ log so
1.0117 1.379 = log , 1.0041 1.282
log (1.379β1.282) = 9.67 years. log (1.0117β1.0041) This model predicts the population of India will exceed that of China in 2026. π‘=
46
Chapter One /SOLUTIONS
54. Let π΄ represent the revenue (in billions of dollars) at Apple π‘ years since 2013. Since π΄ = 54.5 when π‘ = 0 and we want the continuous growth rate, we write π΄ = 54.5πππ‘ . We use the information from 2015, that π΄ = 74.6 when π‘ = 2, to ο¬nd π: 74.6 = 54.5ππβ 2 1.37 = π2π ln(1.37) = 2π π = 0.157. We have π΄ = 54.5π0.157π‘ , which represents a continuous growth rate of 15.7% per year. 55. Let π (π‘) be the world population in billions π‘ years after 2010. (a) Assuming exponential growth, we have
π (π‘) = 6.9πππ‘ .
In 2050, we have π‘ = 40 and we expect the population then to be 9 billion, so 9 = 6.9ππβ 40 . Solving for π, we have ππβ 40 =
9 6.9
) ( 1 9 = 0.00664 = 0.664% per year. ln 40 6.9 (b) The βDay of 8 Billionβ should occur when 8 = 6.9π0.00664π‘ . π=
Solving for π‘ gives 8 6.9 ln(8β6.9) π‘= = 22.277 years. 0.00664
π0.00664π‘ =
So the βDay of 8 Billionβ should be 22.277 years after the end of 2010. This is 22 years and 0.277 β 365 β 101 days; so 101 days into 2032. That is, April 11, 2032. This solution does not take leap years into account. 56. If π was the average yearly inο¬ation rate, in decimals, then 14 (1 + π)3 = 2,400,000, so π = 211.53, i.e. π = 21,153%. 57. If π‘ is time in decades, then the number of vehicles, π , in millions, is given by π = 246(1.155)π‘ . For time π‘ in decades, the number of people, π , in millions, is given by π = 308.7(1.097)π‘ . There is an average of one vehicle per person when
π = 1, or π = π . Thus, we solve for π‘ in the equation: π
246(1.155)π‘ = 308.7(1.097)π‘ , which leads to
(
1.155 1.097
Taking logs on both sides, we get π‘ log so
)π‘
=
(1.155)π‘ 308.7 = (1.097)π‘ 246
308.7 1.155 = log , 1.097 246
log (308.7β246) = 4.41 decades. log (1.155β1.097) This model predicts one vehicle per person in 2054. π‘=
1.4 SOLUTIONS
47
58. For an exponentially growing population, π = π0 πππ‘ , that doubles in π days, we ο¬nd the continuous growth rate π in terms of π. Since π = 2π0 when π‘ = π, we have 2π0 = π0 πππ πππ = 2 ππ = ln 2 1 π = ln 2 π π = π0 π(ln 2)π‘βπ . Doubling time for the phytoplankton population, π , is 0.5 days, and for the foraminifera population, πΉ , it is 5 days. If they both initially have the same population πΆ, then after π‘ days we have π = πΆπ(ln 2)π‘β0.5 = πΆπ1.3863π‘ πΉ = πΆπ(ln 2)π‘β5 = πΆπ0.13863π‘ . (a) We have π = 2πΉ πΆπ1.3863π‘ = 2πΆπ0.13863π‘ π1.3863π‘ = 2π0.13863π‘ 1.3863π‘ = ln 2 + 0.13863π‘ 1.24767π‘ = ln 2 π‘ = 0.556 days. The phytoplankton population is double the foraminifera population after 0.556 days, a little over 13 hours. (b) We have π = 1000πΉ πΆπ
1.3863π‘
= 1000πΆπ0.13863π‘
π1.3863π‘ = 1000π0.13863π‘ 1.3863π‘ = ln 1000 + 0.13863π‘ 1.24767π‘ = ln 1000 π‘ = 5.537 days. The phytoplankton population is 1000 times the foraminifera population after 5.537 days, about ο¬ve and a half days. 59. We assume exponential decay and solve for π using the half-life: πβπ(5730) = 0.5
so
π = 1.21 β 10β4 .
= 0.995,
π‘=
ln 0.995 = 41.43 years. β1.21 β 10β4
Now ο¬nd π‘, the age of the painting: β4 π‘
πβ1.21β 10
so
Since Vermeer died in 1675, the painting is a fake. 60. (a) We ο¬nd an exponential model in the form π(π‘) = π0 ππ‘ . Using π(0) = 25 and π(1) = 21.8, we have π(π‘) = 25ππ‘ 21.8 = 25π1 = 25π. Thus
21.8 = 0.872 25 π(π‘) = 25(0.872)π‘ .
π=
Alternately, we could use π(π‘) = π0 πππ‘ . Then we have 21.8 = 25ππβ 1 = 25ππ , giving ) ( 21.8 = ln(0.872) = β0.136966 π = ln 25 π(π‘) = 25πβ0.136966π‘ .
48
Chapter One /SOLUTIONS (b) We ο¬nd π‘ so that 25(0.872)π‘ = 10, giving 10 25 ( ) 10 π‘ ln(0.872) = ln 25 ln(10β25) π‘= = 6.6899. ln(0.872) (0.872)π‘ =
Alternatively, solving 25πβ0.136966π‘ = 10 gives ln(10β25) = 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 π·(π‘) = π(2π‘), then ( )π‘ π·(π‘) = 25(0.872)2π‘ = 25 0.8722 = 25(0.7604)π‘ . π‘=β
Alternatively,
π·(π‘) = 25πβ0.136966(2π‘) = 25πβ0.273932π‘ .
(d) Starting three years earlier, but with π‘ measured from the original time, we have πΈ(π‘) = π(π‘ + 3), so πΈ(π‘) = 25(0.872)π‘+3 = 25(0.872)3 (0.872)π‘ = 16.576(0.872)π‘ . Alternatively,
πΈ(π‘) = 25πβ0.136966(π‘+3) = 25πβ0.136966(3) πβ0.136966π‘ = 16.576πβ0.136966π‘ .
61. Let π1 be the strength of the ο¬rst earthquake and let π2 be the strength of the second earthquake. Then ( ) π1 π 1 = log = 7.8 π0 ( ) π2 = 7.3. π 2 = log π0 (a) We want to know π1 βπ0 , so we raise the expression for π 1 to the tenth power: π1 = 107.8 = 63,095,734 β 63 million. π0 (b) We want to know π1 βπ2 , so we subtract the two expressions for π 1 and π 2 , giving ( ) ( ) ( ) ( ) π1 βπ0 π1 π2 π1 β log = log = log = 7.8 β 7.3 = 0.5. π 1 β π 2 = log π0 π0 π2 βπ0 π2 To ο¬nd the ratio π1 βπ1 we raise to the tenth power: π1 = 100.5 = 3.162. π2 The ο¬rst earthquake was just over three times as large as the second one. 62. We know that the π¦-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 π (π₯) = 10π₯ at the point π₯ = log 2. The π¦-coordinate of this point is then π¦ = 10π₯ = 10log 2 = 2, so (log 2, 2) is the point of intersection. We can now ο¬nd the slope of the line: π=
2β1 1 = . log 2 β 0 log 2
Plugging this into the point-slope formula for a line, we have π¦ β π¦1 = π(π₯ β π₯1 ) 1 (π₯ β 0) π¦β1 = log 2 1 π¦= π₯ + 1 β 3.3219π₯ + 1. log 2
1.4 SOLUTIONS
49
63. (a) Since π0 = 1 and 100 = 1, we know that logπ 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 logπ 2 β 0.7 (because π0.7 β 2) and log10 2 β 0.3 (because 100.3 β 2), so A is logπ π₯ and B is log10 π₯. For 0 < π₯ < 1, say π₯ = 0.5, we have logπ 0.5 β β0.7 and log10 0.5 β β0.3, so C is log10 π₯ and D is logπ π₯. 64. The function ππ₯ has a vertical intercept of 1, so must be π΄. The function ln π₯ has an π₯-intercept of 1, so must be π·. The graphs of π₯2 and π₯1β2 go through the origin. The graph of π₯1β2 is concave down so it corresponds to graph πΆ and the graph of π₯2 is concave up so it corresponds to graph π΅. 65. Since π = π0 πππ‘ , the doubling time, π , is given by 2π0 = π0 πππ ln 2 π = . π Thus, doubling π does not double π ; 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 π. Since ln π = 1, ln2 π = 12 = 1, but ln(ln(π)) = ln(1) = 0. See the graphs in Figure 1.40. (Note that ln(ln(π₯)) is only deο¬ned for π₯ > 1.)
2 1 β1
1
π (π₯) = ln π₯ 1
2
3
4
5
β1 β2
2
π (π₯) = ln(ln π₯) 1
2
3
1 4
π (π₯) = ln2 π₯
5 1
2
3
4
5
Figure 1.40 67. (a) The π¦-intercept of β(π₯) = ln(π₯ + π) is β(0) = ln π. Thus increasing π increases the π¦-intercept. (b) The π₯-intercept of β(π₯) = ln(π₯ + π) is where β(π₯) = 0. Since this occurs where π₯ + π = 1, or π₯ = 1 β π, increasing π moves the π₯-intercept to the left. 68. The vertical asymptote is where π₯ + π = 0, or π₯ = βπ. Thus increasing π moves the vertical asymptote to the left. 69. (a) The π¦-intercept of π(π₯) = ln(ππ₯ + 2) is π(0) = ln 2. Thus increasing π does not eο¬ect the π¦-intercept. (b) The π₯-intercept of π(π₯) = ln(ππ₯ + 2) is where π(π₯) = 0. Since this occurs where ππ₯ + 2 = 1, or π₯ = β1βπ, increasing π moves the π₯-intercept toward the origin. (The intercept is to the left of the origin if π > 0 and to the right if π < 0.) 70. The vertical asymptote is where π₯ + 2 = 0, or π₯ = β2, so increasing π does not eο¬ect the vertical asymptote. 71. The vertical asymptote is where ππ₯ + 2 = 0, or π₯ = β2βπ. Thus increasing π moves the vertical asymptote toward the origin. (The asymptote is to the left of the origin for π > 0 and to the right of the origin for π < 0.) 72. Properties of logs give
ln(π0 πππ‘ ) = ln π0 + ln πππ‘ = ln π0 + ππ‘.
Therefore ln(π0 πππ‘2 ) β ln(π0 πππ‘1 ) ln π (π‘2 ) β ln π (π‘1 ) = π‘2 β π‘1 π‘2 β π‘1 ln π0 + ππ‘2 β ln π0 β ππ‘1 = π‘2 β π‘1 π(π‘2 β π‘1 ) = = π. π‘2 β π‘1
Strengthen Your Understanding 73. The function β log |π₯| is even, since | β π₯| = |π₯|, which means β log | β π₯| = β 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(π΄π΅) = ln π΄ + ln π΅. We may also check that the given property is not correct by taking π΄ = π΅ = 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(π΄π΅) = ln π΄ + ln π΅. There is no property of logarithms that states the logarithm of a sum is the sum of logarithms. We can check by taking π΄ = π΅ = 1. Then the statement gives us the incorrect statement: ln 2 = ln 1 + ln 1 = 0. 78. The functions π¦ = ln π₯ and π¦ = ππ₯ are inverses of each other, but not reciprocals of each other. As their graphs show, π¦ = 1β ln π₯ and π¦ = ππ₯ donβt even have the same domain. 79. The function π¦ = 0.7 log π₯ works, as it scales down each value of π¦ = log π₯ for π₯ > 1. The graph of π¦ = 0.7 log π₯ is below the graph of π¦ = log π₯ as long as π₯ > 1. 80. One possibility is π (π₯) = βπ₯, because ln(βπ₯) is only deο¬ned if βπ₯ > 0. 81. One possibility is π (π₯) = ln(π₯ β 3). 82. True, as seen from the graph. 83. False, since log(π₯ β 1) = 0 if π₯ β 1 = 1, so π₯ = 2. 84. False. The inverse function is π¦ = 10π₯ . 85. False, since ππ₯ + π = 0 if π₯ = βπβπ. Thus π¦ = ln(ππ₯ + π) has a vertical asymptote at π₯ = βπβπ.
Solutions for Section 1.5 EXERCISES 1. See Figure 1.41.
) 3π = β1 is negative. 2 ( ) 3π cos =0 2 ( ) 3π tan is undeο¬ned. 2 sin
(
-
Figure 1.41
1.5 SOLUTIONS 2. See Figure 1.42. sin(2π) = 0 cos(2π) = 1 is positive. tan(2π) = 0
6
Figure 1.42 3. See Figure 1.43. π 4 π cos 4 π tan 4 sin
is positive is positive is positive
I
Figure 1.43 4. See Figure 1.44. sin 3π = 0 cos 3π = β1 is negative tan 3π = 0
?
Figure 1.44
51
52
Chapter One /SOLUTIONS 5. See Figure 1.45.
( ) π is positive. 6 ( ) π cos is positive. 6 ( ) π tan is positive. 6 sin
M
Figure 1.45 6. See Figure 1.46. 4π 3 4π cos 3 4π tan 3 sin
is negative is negative is positive
j
Figure 1.46 7. See Figure 1.47.
) β4π is positive. 3 ) ( β4π is negative. cos 3 ) ( β4π is negative. tan 3 sin
(
*
Figure 1.47
1.5 SOLUTIONS 8. 4 radians β
180β¦ = π radians
(
720 π
)β¦
53
β 240β¦ . See Figure 1.48. sin 4
is negative
cos 4
is negative
tan 4
is positive.
j
Figure 1.48 9. β1 radian β
180β¦
π radians
=β
(
180β¦ π
)
β β60β¦ . See Figure 1.49. sin (β1)
is negative
cos (β1)
is positive
tan (β1)
is negative.
Figure 1.49 10. The period is 2πβ3, because when π‘ varies from 0 to 2πβ3, the quantity 3π‘ varies from 0 to 2π. The amplitude is 7, since the value of the function oscillates between β7 and 7. 11. The period is 2πβ(1β4) = 8π, because when π’ varies from 0 to 8π, the quantity π’β4 varies from 0 to 2π. The amplitude is 3, since the function oscillates between 2 and 8. 12. The period is 2πβ2 = π, because as π₯ varies from βπβ2 to πβ2, the quantity 2π₯ + π varies from 0 to 2π. The amplitude is 4, since the function oscillates between 4 and 12. 13. The period is 2πβπ = 2, since when π‘ increases from 0 to 2, the value of ππ‘ increases from 0 to 2π. 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 and amplitude 2, so it is given by π (π₯) = 2 sin 4 ( ) π₯ . 15. This graph is a cosine curve with period 6π and amplitude 5, so it is given by π (π₯) = 5 cos 3 16. This graph is an inverted sine curve with amplitude 4 and period π, so it is given by π (π₯) = β4 sin(2π₯). ( ) π₯ . 17. This graph is an inverted cosine curve with amplitude 8 and period 20π, so it is given by π (π₯) = β8 cos 10 18. This graph has period 6, amplitude 5 and no vertical or horizontal shift, so it is given by ( ) ( ) 2π π π (π₯) = 5 sin π₯ = 5 sin π₯ . 6 3 19. The graph is a cosine curve with period 2πβ5 and amplitude 2, so it is given by π (π₯) = 2 cos(5π₯).
54
Chapter One /SOLUTIONS
20. The graph is an inverted sine curve with amplitude 1 and period 2π, shifted up by 2, so it is given by π (π₯) = 2 β sin π₯. 21. This can be represented by a sine function of amplitude 3 and period 18. Thus, ( ) π π₯ . π (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 2π π₯ = 3 + 3 sin π₯ . π (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 π (π₯) = 2 sin
24.
π 5
M
) ( π π = cos cos β (by picture) 5 5 = 0.809.
π 5
25. (0,1) π 5
1
sin π5 cos π5
sin π5
(1,0)
cos π5
By the Pythagorean Theorem, (cos π5 )2 + (sin π5 )2 = 12 ; β β so (sin π5 )2 = 1 β (cos π5 )2 , and sin π5 = 1 β (cos π5 )2 = 1 β (0.809)2 β 0.588.
26.
We take the positive square root since by the picture we know that sin π5 is positive. (0,1)
π sin 12
π cos 12
π cos 12 π 12
(1,0)
β
π sin 12
1
π 2 π 2 π 2 π 2 π By the Pythagorean Theorem, (cos 12 ) + (sin 12 ) = 12 ; so (cos 12 ) = 1 β (sin 12 ) and cos 12 =
β π 2 1 β (sin 12 ) =
π 1 β (0.259)2 β 0.966. We take the positive square root since by the picture we know that cos 12 is positive.
1.5 SOLUTIONS ) ( ) ( π π = β sin = β0.259. 27. Since sin π is an odd function, sin β 12 12 π ο¬rst. We can use the Pythagorean identity sin2 π + cos2 π = 1 to ο¬nd 28. Since tan π = sin πβ cos π, we need to ο¬nd cos 12 β π cos = Β± 1 β 0.2592 = Β±0.966. 12 π Since the angle π = lies in the ο¬rst quadrant, cos π = 0.966. Thus, 12 tan
π 0.259 = = 0.268. 12 0.966
π ο¬rst. We can use the Pythagorean identity sin2 π + cos2 π = 1 to ο¬nd 5 β π sin = Β± 1 β 0.8092 = Β±0.588. 5
29. Since tan π = sin πβ cos π, we need to ο¬nd sin
Since the angle π =
π lies in the ο¬rst quadrant, sin π5 = 0.588. Thus, 5 tan
0.588 π = = 0.727. 5 0.809
30. We ο¬rst divide by 5 and then use inverse sine: 2 = sin(3π₯) 5 β1 sin (2β5) = 3π₯ π₯=
sinβ1 (2β5) β 0.1372. 3
There are inο¬nitely many other possible solutions since the sine is periodic. 31. We ο¬rst isolate cos(2π₯ + 1) and then use inverse cosine: 1 = 8 cos(2π₯ + 1) β 3 4 = 8 cos(2π₯ + 1) 0.5 = cos(2π₯ + 1) cosβ1 (0.5) = 2π₯ + 1 cosβ1 (0.5) β 1 π₯= β 0.0236. 2 There are inο¬nitely many other possible solutions since the cosine is periodic. 32. We ο¬rst isolate tan(5π₯) and then use inverse tangent: 8 = 4 tan(5π₯) 2 = tan(5π₯) tanβ1 2 = 5π₯ tanβ1 2 π₯= = 0.221. 5 There are inο¬nitely many other possible solutions since the tangent is periodic. 33. We ο¬rst isolate (2π₯ + 1) and then use inverse tangent: 1 = 8 tan(2π₯ + 1) β 3 4 = 8 tan(2π₯ + 1) 0.5 = tan(2π₯ + 1) arctan(0.5) = 2π₯ + 1 arctan(0.5) β 1 π₯= = β0.268. 2 There are inο¬nitely many other possible solutions since the tangent is periodic.
55
56
Chapter One /SOLUTIONS
34. We ο¬rst isolate sin(5π₯) and then use inverse sine: 8 = 4 sin(5π₯) 2 = sin(5π₯). But this equation has no solution since β1 β€ sin(5π₯) β€ 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 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 radians and 1 minute = 60 seconds, we have 200
rev rad 1 rad = (200) β 2π = 200 β 2π min min 60 sec (200)(6.283) β 60 β 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 = arctan(1β12) = 0.0831. To ο¬nd the angle in degrees, multiply by 180βπ. Hence 1 180 arctan = 4.76β¦ . π= π 12 (b) We have 180 1 π= arctan = 7.13β¦ . π 8 (c) We have 180 1 π= arctan = 2.86β¦ . π 20 1 ft
π π₯ ft
Figure 1.50
PROBLEMS 40. (a) The period is 2π. (b) After π, the values of cos 2π repeat, but the values of 2 sin π do not (in fact, they repeat but ο¬ipped over the x-axis). After another π, that is after a total of 2π, the values of cos 2π repeat again, and now the values of 2 sin π repeat also, so the function 2 sin π + 3 cos 2π repeats at that point. 41. All three functions have amplitude 2 and period 2π. Each is just a horizontal shift of the others. (a) We see that β(π‘) looks like a cosine graph with amplitude 2 and period 2π, but shifted right by πβ2. Thus, β(π‘) = 2 cos (π‘ β πβ2). (b) We see that π (π‘) has and amplitude of 2 and a period of 2π. Furthermore, since π (0) = 2, we know that π (π‘) = 2 cos π‘. (c) We see that π(π‘) looks like a cosine graph with amplitude 2 and period 2π, but shifted left by πβ2. Thus, π(π‘) = 2 cos (π‘ + πβ2). 42. (a) The parameter π΄ is the amplitude of the function. Since the functions oscillate between β20 and +20, we have π΄ = 20. (b) We have π΅ = 2πβπ , where π is the period of the function. From the graphs, we see that the function repeats every 100 units, so the period is 100. Thus π΅ = 2πβ100 = 0.0628. (c) Since cos π‘ has a maximum at π‘ = 0, the function π΄ cos((2πβ100)π‘) also achieves its maximum at π‘ = 0. Thus β = 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, can be determined by checking how far the ο¬rst 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 = 60. Similarly, graph (III) corresponds to β = 20 and graph (IV) to β = 50.
1.5 SOLUTIONS
57
43. The graph is a stretched sine function, so it starts at the midline, π¦ = 0, when π₯ = 0. The amplitude is π, so the sinusoidal graph oscillates between a minimum of βπ and a maximum of π. Since π is positive, the function begins by increasing. The period is 2π. See Figure 1.51. π¦ 2π
π β2π
2π π
βπ
π₯
β2π
Figure 1.51 44. The graph is a stretched cosine function reο¬ected 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 βπ and a maximum of π. The period is 2π. See Figure 1.52. π¦ 2π
π
β2π
2π π
βπ
π₯
β2π
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 ο¬nding 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 β π = 0 and a maximum of π + π = 2π. The period is 2π. See Figure 1.53. π¦ 2π
π β2π
βπ
π
β2π
Figure 1.53
2π
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 ο¬nding the midline, which is βπ, since the sine function is shifted up by βπ (down by π). The amplitude is π, so the sinusoidal graph oscillates between a minimum of βπ β π = β2π and a maximum of βπ + π = 0. Since π is positive, the function begins by increasing. The period is 2π. See Figure 1.54. π¦ 2π
π
β2π
2π π
βπ
π₯
β2π
Figure 1.54 47. The graph is a stretched sine function shifted horizontally. Since we have sin(π₯ β 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 βπ and a maximum of π. Since π is positive, the function is increasing at π₯ = π. The period is 2π. See Figure 1.55. π¦ 2π
π
β2π
2π
βπ
π
π₯
β2π
Figure 1.55 48. The graph is a stretched cosine function shifted horizontally. Since we have cos(π₯ + π), the function is shifted βπ units to the right, which is π units to the left, so the function takes on its maximum value when π₯ = βπ. The amplitude is π, so the sinusoidal graph oscillates between a minimum of βπ and a maximum of π. The period is 2π. See Figure 1.56. π¦ 2π
π
β2π βπ
β2π
Figure 1.56
2π
π₯
1.5 SOLUTIONS
59
49. The graph is a vertically stretched sine function horizontally compressed by a factor of 2πβπ. 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 βπ and a maximum of π. Since π is positive, the function is increasing at π₯ = 0. The period is 2πβ(2πβπ) = π. See Figure 1.57. π¦ 2π
π βπ
β2π
π
2π
π₯
β2π
Figure 1.57 50. (a) Since πΆ represents the vertical shift, πΆ = 27.5β¦ C, the average temperature. (b) The amplitude, π΄, is the distance above and below the midline at πΆ, which represents the temperature variation above and below the average. Since the data rises 36.7 β 27.5 = 9.2β¦ C above 27.5β¦ C, and falls 27.5 β 18.4 = 9.1β¦ C. We take π΄ to be the average 9.2 + 9.1 = 9.15β¦ C. π΄= 2 (c) Since the period is 12 months, 2π 12 = π΅ so π΅ = πβ6. (d) The function is ( ) π π + 27.5. π»(π) = 9.15 cos 6 See Figure 1.58. temperature (β¦ C) 36.7 27.5 18.4
1
3
5
7
9
11
π (months)
Figure 1.58 51. The parameter πΆ 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. πΆ= 2 52. The parameter π΄ gives the amplitude of the oscillation. The midline is at about 18 and the maximum is about 30, so the amplitude is the diο¬erence π΄ = 30 β 18 = 12β¦ C. 53. We have π΅ = 2πβπ where π is the period of the function. Since the period is 12 months, we have π΅ = 2πβ12 = πβ6.
60
Chapter One /SOLUTIONS
54. Since the maximum value of the function appears at about π‘ = 7.5, we see that the graph is obtained by horizontally shifting the graph of π΄ cos(π΅π‘) + πΆ to the right by 7.5 units. Thus β = 7.5 months. 55. The parameter πΆ 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 βsec. πΆ= 2 56. The parameter π΄ gives the amplitude of the oscillation. The midline is about 450 and the maximum is about 725; the amplitude is the diο¬erence. Thus π΄ = 725 β 450 = 275 thousand ft3 βsec. 57. We have π΅ = 2πβπ where π is the period of the function. Since the period is 12 months, we have π΅ = 2πβ12 = πβ6. 58. Since the graph increases across the midline at about π‘ = 1, we see that it is obtained by horizontally shifting the graph π΄ sin(π΅π‘) + πΆ to the right by 1 unit. Thus β = 1 month. 59. Over the one-year period, the average value is about 75β¦ and the amplitude of the variation is about 90β60 = 15β¦ . The 2 function assumes its minimum value right at the beginning of the year, so we want a negative cosine function. Thus, for π‘ in years, we have the function ) ( 2π π‘ . π (π‘) = 75 β 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₯ ο¬rst and then take the sine. sin2 π₯ = (sin π₯)2 means ο¬nd sin π₯ and then square it. sin(sin π₯) means ο¬nd sin π₯ and then take the sine of that. Expressing each as a composition: If π (π₯) = sin π₯ and π(π₯) = π₯2 , then 2 sin π₯ = π (π(π₯)) sin2 π₯ = π(π (π₯)) sin(sin π₯) = π (π (π₯)). 61. Suppose π is at the point (3πβ2, β1) and π is at the point (5πβ2, 1). Then Slope =
1 β (β1) 2 = . 5πβ2 β 3πβ2 π
If π had been picked to the right of π, the slope would have been β2βπ. 62. (a) See Figure 1.59.
900
π
800 700 100 Jan. 1
Jul. 1
Jan. 1
π‘ (months)
Figure 1.59 = 800, amplitude = 900β700 = 100, and period = 12 months, so π΅ = 2πβ12 = (b) Average value of population = 700+900 2 2 πβ6. Since the population is at its minimum when π‘ = 0, we use a negative cosine: ( ) ππ‘ . π = 800 β 100 cos 6
1.5 SOLUTIONS 63. We use a cosine of the form
61
π» = π΄ cos(π΅π‘) + πΆ
and choose π΅ so that the period is 24 hours, so 2πβπ΅ = 24 giving π΅ = πβ12. The temperature oscillates around an average value of 60β¦ F, so πΆ = 60. The amplitude of the oscillation is 20β¦ F. To arrange that the temperature be at its lowest when π‘ = 0, we take π΄ negative, so π΄ = β20. Thus ( ) π π΄ = 60 β 20 cos π‘ . 12 64. The depth function is a vertical shift of a function of the form π΄ sin(π΅π‘). The vertical shift is π΄ = (5.5 + 8.5)β2 = 7. The amplitude is π΄ = 8.5 β 7 = 1.5. The period is 6 = 2πβπ΅ so π΅ = 2πβ6 = πβ3. Thus, we have ( ) π π‘ . Depth = 7 + 1.5 sin 3 65. (a) Beginning at time π‘ = 0, the voltage will have oscillated through a complete cycle when cos(120ππ‘) = cos(2π), hence when π‘ = 601 second. The period is 601 second. (b) π0 represents the amplitude of the oscillation. (c) See Figure 1.60. π π0
1 120
1 60
π‘
Figure 1.60
66. (a) When the time is π‘ hours after 6 am, the solar panel outputs π (π‘) = π (π(π‘)) watts. So, ( ) π π (π‘) = 10 sin π‘ 14 where 0 β€ π‘ β€ 14 is the number of hours after 6 am. (b) The graph of π (π‘) is in Figure 1.61: π (watts) 10
7
14
π‘ (hrs after 6 am)
Figure 1.61 (c) The power output is greatest when sin(ππ‘β14) = 1. Since 0 β€ ππ‘β14 β€ π, the only point in the domain of π at which sin(ππ‘β14) = 1 is when ππ‘β14 = πβ2. Therefore, the power output is greatest when π‘ = 7, that is, at 1 pm. The output at this time will be π (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 π‘ is the number of hours since 8 am, the angle between a solar panel and the sun is π=
π 14 π= π‘ 9 9
where 0 β€ π‘ β€ 9.
The solar panel outputs π(π‘) = π (π(π‘)) watts: π(π‘) = 10 sin
(
π π‘ 9
)
where 0 β€ π‘ β€ 9 is the number of hours after 8 am. 67. The function π has period of π, so its graph is as shown in Figure 1.62. The maximum value of the range is π£20 βπ and occurs when π = πβ4.
π£20
π π£2
π
π = π0 sin 2π
π 4
π 2
π
Figure 1.62
68. (a) π (π‘) = β0.5 + sin π‘, π(π‘) = 1.5 + sin π‘, β(π‘) = β1.5 + sin π‘, π(π‘) = 0.5 + sin π‘. (b) The values of π(π‘) are one more than the values of π(π‘), so π(π‘) = 1 + π(π‘). This happens because π(π‘) = 1.5 + sin π‘ = 1 + 0.5 + sin π‘ = 1 + π(π‘). (c) Since β1 β€ sin π‘ β€ 1, adding 1.5 everywhere we get 0.5 β€ 1.5 + sin π‘ β€ 2.5 and since 1.5 + sin π‘ = π(π‘), we get 0.5 β€ π(π‘) β€ 2.5. Similarly, β2.5 β€ β1.5 + sin π‘ = β(π‘) β€ β0.5. 69. (a) The period of the tides is 2πβ0.5 = 4π = 12.566 hours. (b) The boat is aο¬oat provided the water is deeper than 2.5 meters, so we need π(π‘) = 5 + 4.6 sin(0.5π‘) > 2.5. Figure 1.63 is a graph of π(π‘), with time π‘ in hours since midnight, 0 β€ π‘ β€ 24. The boat leaves at π‘ = 12 (midday). To ο¬nd the latest time the boat can return, we need to solve the equation π(π‘) = 5 + 4.6 sin(0.5π‘) = 2.5. A quick way to estimate the solution is to trace along the line π¦ = 2.5 in Figure 1.63 until we get to the ο¬rst point of intersection to the right of π‘ = 12. The value we want is about π‘ = 20. Thus the water remains deep enough until about 8 pm. To ο¬nd π‘ analytically, we solve 5 + 4.6 sin(0.5π‘) = 2.5 2.5 = β0.5435 sin(0.5π‘) = β 4.6 1 arcsin(β0.5435) = β1.149. π‘= 0.5 This is the value of π‘ immediately to the left of the vertical axis. The water is also 2.5 meters deep one period later at π‘ = β1.149 + 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, π(π‘) was a maximum) when π‘ = 12.566β4 = 3.142. From the ο¬gure, 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 π‘ that we want is π‘ = 11.417 + 2 β 4.291 = 19.999.
1.5 SOLUTIONS depth in meters
63
π(π‘)
10 7.5 5 2.5 5
10
15
20
25
π‘, hours since midnight
Figure 1.63 70. (a) π· = the average depth of the water. (b) π΄ = the amplitude = 15β2 = 7.5. (c) Period = 12.4 hours. Thus (π΅)(12.4) = 2π so π΅ = 2πβ12.4 β 0.507. (d) πΆ is the time of a high tide. 71. Since π is a positive constant, π is a vertical shift of sin π‘ where the midline lies above the π‘-axis. So π matches Graph πΆ. Function π is the sum of sin π‘ plus a linear function ππ‘ + π. We suspect then that the graph of π might periodically oscillate about a line ππ‘ + π, just like the graph of sin π‘ oscillates about its midline. When adding ππ‘ + π to sin π‘, we note that every zero of sin π‘, (π‘, 0), gets displaced to a corresponding point (π‘, ππ‘ + π) that lies both on the graph of π, and on the line ππ‘ + π. See Figure 1.64. So π matches Graph π΅. Function β is the sum of sin π‘ plus an increasing exponential function πππ‘ + π. We suspect then that the graph of π might periodically oscillate about the graph of πππ‘ + π, just like the graph of sin π‘ oscillates about its midline. When adding πππ‘ + π to sin π‘, we note that every zero of sin π‘, (π‘, 0), gets displaced to a corresponding point (π‘, πππ‘ + π) that lies both on the graph of β, and on the graph of πππ‘ + π. See Figure 1.64. So β matches Graph π΄. Note that the oscillations on the graph of β may not be visible for all π‘ values. Function π is the sum of sin π‘ plus a decreasing exponential function βπππ‘ + π. We suspect then that the graph of π might periodically oscillate about the graph of βπππ‘ +π, just like the graph of sin π‘ oscillates about its midline. When adding βπππ‘ + π to sin π‘, we note that every zero of sin π‘, (π‘, 0), gets displaced to a corresponding point (π‘, βπππ‘ + π) that lies both on the graph of π, and on the graph of βπππ‘ + π. See Figure 1.64. So π matches Graph π·. Note that the oscillations on the graph of π may not be visible for all π‘ values. π΄ π΅ (π‘, πππ‘ + π) (π‘, ππ‘ + π) πΆ (π‘, βπππ‘ + π)
π· (π‘, 0)
π‘
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 diο¬erence between these two values, 410 β 398 = 12, gives the overall increase. (b) The average rate of increase is given by Average monthly increase of monthly mean =
1 410 β 398 = ppm/month. 60 β 0 5
64
Chapter One /SOLUTIONS This tells us that the slope of a linear equation approximating the black curve is 1β5. Since the vertical intercept is about 398, a possible equation for the approximately linear black curve is π¦=
1 π‘ + 398, 5
where π‘ 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 π¦ = 3.5 sin π‘ . 6 ( ) 1 π π‘ and π(π‘) = π‘ + 398, we have (d) Taking π (π‘) = 3.5 sin 6 5 ( ) 1 π β(π‘) = 3.5 sin π‘ + π‘ + 398. 6 5 See Figure 1.65. ppm 415 410 405 400 395
12
24
36
48
π‘ (months since Dec 2013)
60
Figure 1.65
73. Figure 1.66 shows that the cross-sectional area is one rectangle of area βπ€ and two triangles. Each triangle has height β and base π₯, where β β = tan π so π₯ = . π₯ tan π 1 β2 Area of triangle = π₯β = 2 2 tan π Total area = Area of rectangle + 2(Area of triangle) β2 β2 = βπ€ + . = βπ€ + 2 β 2 tan π tan π
π₯π
π
6
π₯6π
β
β
?
π€
?π
Figure 1.66
74. (a) Two solutions: 0.4 and 2.7. See Figure 1.67. (b) arcsin(0.4) is the ο¬rst solution approximated above; the second is an approximation to π β arcsin(0.4). (c) By symmetry, there are two solutions: β0.4 and β2.7.
1.5 SOLUTIONS
65
(d) β0.4 β β arcsin(0.4) and β2.7 β β(π β arcsin(0.4)) = arcsin(0.4) β π. π¦ 1 0.4 β2.7
β0.4 0.4
π₯
2.7
β0.4 β1
Figure 1.67 75. (a) A table of values for π(π₯) is: π₯
β1
β0.8
β0.6
β0.4
β0.2
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
π¦ = arccos π₯
π¦
6 Range
π 2
β1
1
Domain
-
? π₯
Figure 1.68 1
βπβ2
π¦ π¦ = cos π₯
πβ2
π
π₯
β1
Figure 1.69 (c) The domain of arccos is β1 β€ π₯ β€ 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 π¦ = arccos π₯ is 0 β€ π β€ π. (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 [β π2 , π2 ]. Hence, the range of the arcsine is [β π2 , π2 ]. But the piece of the cosine having domain [β π2 , π2 ] does not have an inverse, because there are horizontal lines that intersect its graph twice. Instead, we deο¬ne arccosine to be the inverse of the piece of cosine having domain [0, π], so the range of arccosine is [0, π], which is diο¬erent from the range of arcsine. See Figure 1.69.
Strengthen Your Understanding 76. Scaling the output (that is, the function values, as in π¦ = 3 cos π₯) does not change the period but changes the amplitude. Scaling the input (that is, the independent variable, as in π¦ = cos 3π₯) changes the period of the function but not the amplitude. So π has the same period, 2π, as cos π₯, but π has a period smaller than 2π. See Figure 1.70.
66
Chapter One /SOLUTIONS π (π₯) = 3 cos π₯
3 2 1 0 β1 β2 β3
π(π₯) = cos 3π₯ 2π
4π
π₯
Figure 1.70
77. Increasing the value of π΅ decreases the period. For example, π (π₯) = sin π₯ has period 2π, whereas π(π₯) = sin(2π₯) has period π. 78. The functions π (π₯) = sin π₯ and π(π₯) = cos π₯ both have period 2π. The product, π π, of these two functions is periodic, but has a smaller period, π. See Figure 1.71. π¦ 1
π¦ = sin π₯ β cos π₯
π
2π
π₯ 3π
β1
Figure 1.71
79. The maximum value of π΄ sin(π΅π₯) is π΄, so the maximum value of π¦ = π΄ sin(π΅π₯) + πΆ is π¦ = π΄ + πΆ. 80. For π΅ > 0, the period of π¦ = sin(π΅π₯) is 2πβπ΅. Thus, we want 2π = 23 π΅
so
π΅=
2π . 23
The function is π (π₯) = sin(2ππ₯β23) 81. The midline is π¦ = (1200 + 2000)β2 = 1600 and the amplitude is π¦ = (2000 β 1200)β2 = 400, so a possible function is π (π₯) = 400(cos π₯) + 1600. 82. True. All functions in this family have period 2π since the independent variable, π₯, (the input) is not scaled by a constant. The constant π 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, the period of the corresponding function in the family is 2πβπ. 84. False. The function cos π is decreasing and the function sin π is increasing. Thus, the function β sin π is decreasing over this interval, which means π is decreasing. 85. False. The period is 2πβ(0.05π) = 40 86. True. The period is 2πβ(200π) = 1β100 seconds. Thus, the function executes 100 cycles in 1 second. 87. False. If π = πβ2, 3πβ2, 5πβ2 β¦, then π β πβ2 = 0, π, 2π β¦, and the tangent is deο¬ned (it is zero) at these values. 88. False. When π₯ < 0, we have sin |π₯| = sin(βπ₯) = β sin π₯ β sin π₯. 89. False. When π < π₯ < 2π, we have sin |π₯| = sin π₯ < 0 but | sin π₯| > 0. 90. False. When πβ2 < π₯ < 3πβ2, we have cos |π₯| = cos π₯ < 0 but | cos π₯| > 0. 91. True. Since cos(βπ₯) = cos π₯, cos |π₯| = cos π₯. 92. False. For example, sin(0) β sin((2π)2 ), since sin(0) = 0 but sin((2π)2 ) = 0.98. 93. True. Since sin(π + 2π) = sin π for all π, we have π(π + 2π) = πsin(π+2π) = πsin π = π(π) for all π.
1.6 SOLUTIONS
67
94. False. A counterexample is given by π (π₯) = sin π₯, which has period 2π, and π(π₯) = π₯2 . The graph of π (π(π₯)) = sin(π₯2 ) in Figure 1.72 is not periodic with period 2π.
1 β2π
βπ
π¦
β1
π (π₯) π
2π
π₯
Figure 1.72 95. True. If π(π₯) has period π, then π(π₯ + π) = π(π₯). Thus we have π (π(π₯ + π)) = π (π(π₯)) which shows that π (π(π₯)) is periodic with period π. 96. True, since | sin(βπ₯)| = | β sin π₯| = sin π₯. 97. False. If π‘ < βπβ2 or π‘ > πβ2, then sinβ1 (sin π‘) β π‘. Note, however, that sinβ1 (sin π‘) = π‘ for βπβ2 β€ π‘ β€ πβ2. 98. True. Since sin(π‘ + 2π) = sin π‘, we have π (π‘ + 2π) = sinβ1 (sin(π‘ + 2π)) = sinβ1 (sin π‘) = π (π‘). To see that this is the smallest interval on which we have a complete cycle, notice that since π (π‘) = 0 only for π‘ = ππ, π = 0, Β±1, Β±2, β¦, the only possible period shorter than 2π would be π. But π (πβ2)) = πβ2 and π (πβ2 + π) = βπβ2. Thus, π is not a period.
Solutions for Section 1.6 EXERCISES 1. As π₯ β β, π¦ β β. As π₯ β ββ, π¦ β ββ. 2. As π₯ β β, π¦ β β. As π₯ β ββ, π¦ β 0. 3. Since π (π₯) is an even power function with a negative leading coeο¬cient, it follows that π (π₯) β ββ as π₯ β +β and π (π₯) β ββ as π₯ β ββ. 4. Since π (π₯) is an odd power function with a positive leading coeο¬cient, it follows that π (π₯) β +β as π₯ β +β and π (π₯) β ββ as π₯ β ββ. 5. As π₯ β Β±β, the lower-degree terms of π (π₯) become insigniο¬cant, and π (π₯) becomes approximated by the highest degree term of 5π₯4 . Thus, as π₯ β Β±β, we see that π (π₯) β +β. 6. As π₯ β Β±β, the lower-degree terms of π (π₯) become insigniο¬cant, and π (π₯) becomes approximated by the highest degree term of β5π₯3 . Thus, as π₯ β +β, we see that π (π₯) β ββ and as π₯ β ββ, we see that π (π₯) β +β. 7. As π₯ β Β±β, the lower-degree terms of π (π₯) become insigniο¬cant, and π (π₯) becomes approximated by the highest degree 3π₯2 terms in the numerator and denominator. Thus, as π₯ β Β±β, we see that π (π₯) behaves like 2 = 3. We have π (π₯) β 3 π₯ as π₯ β Β±β. 8. As π₯ β Β±β, the lower-degree terms of π (π₯) become insigniο¬cant, and π (π₯) becomes approximated by the highest degree β3π₯3 = β3β2. We have terms in the numerator and denominator. Thus, as π₯ β Β±β, we see that π (π₯) behaves like 2π₯3 π (π₯) β β3β2 as π₯ β Β±β. 9. As π₯ β Β±β, we see that 3π₯β4 gets closer and closer to 0, so π (π₯) β 0 as π₯ β Β±β. 10. As π₯ β +β, we have π (π₯) β +β. As π₯ β ββ, we have π (π₯) β 0. 11. The power function with the higher power dominates as π₯ β β, so 0.2π₯5 is larger.
68
Chapter One /SOLUTIONS
12. An exponential growth function always dominates a power function as π₯ β β, so 10π0.1π₯ is larger. 13. An exponential growth function always dominates a power function as π₯ β β, so 1.05π₯ is larger. 14. The lower-power terms in a polynomial become insigniο¬cant as π₯ β 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 β, so 2π₯4 is larger. 15. The lower-power terms in a polynomial become insigniο¬cant as π₯ β 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 β, so the polynomial with leading term 3π₯5 is larger. As π₯ β β, we see that 25 β 40π₯2 + π₯3 + 3π₯5 is larger. β 16. A power function with positive exponent dominates a log function, so as π₯ β β, we see that π₯ is larger. 17. (I) (a) Minimum degree is 3 because graph turns around twice. (b) Leading coeο¬cient is negative because π¦ β ββ as π₯ β β. (II) (a) Minimum degree is 4 because graph turns around three times. (b) Leading coeο¬cient is positive because π¦ β β as π₯ β β. (III) (a) Minimum degree is 4 because graph turns around three times. (b) Leading coeο¬cient is negative because π¦ β ββ as π₯ β β. (IV) (a) Minimum degree is 5 because graph turns around four times. (b) Leading coeο¬cient is negative because π¦ β ββ as π₯ β β. (V) (a) Minimum degree is 5 because graph turns around four times. (b) Leading coeο¬cient is positive because π¦ β β as π₯ β β. 18. (a) From the π₯-intercepts, we know the equation has the form π¦ = π(π₯ + 2)(π₯ β 1)(π₯ β 5). Since π¦ = 2 when π₯ = 0, 2 = π(2)(β1)(β5) = π β 10 1 π= . 5 Thus we have
1 (π₯ + 2)(π₯ β 1)(π₯ β 5). 5 19. (a) Because our cubic has a root at 2 and a double root at β2, it has the form π¦=
π¦ = π(π₯ + 2)(π₯ + 2)(π₯ β 2). Since π¦ = 4 when π₯ = 0, 4 = π(2)(2)(β2) = β8π, 1 π=β . 2 Thus our equation is
1 π¦ = β (π₯ + 2)2 (π₯ β 2). 2
20. π (π₯) = π(π₯ + 3)(π₯ β 1)(π₯ β 4) = π(π₯3 β 2π₯2 β 11π₯ + 12), where π < 0. (π β β 16 if the horizontal and vertical scales are equal; otherwise one canβt tell how large π is.) 21. π (π₯) = ππ₯(π₯ + 3)(π₯ β 4) = π(π₯3 β π₯2 β 12π₯), where π < 0. (π β β 29 if the horizontal and vertical scales are equal; otherwise one canβt tell how large π is.) 22. π (π₯) = π(π₯ + 2)(π₯ β 1)(π₯ β 3)(π₯ β 5) = π(π₯4 β 7π₯3 + 5π₯2 + 31π₯ β 30), where π > 0. (π β 151 if the horizontal and vertical scales are equal; otherwise one canβt tell how large π is.) 23. π (π₯) = π(π₯ + 2)(π₯ β 2)2 (π₯ β 5) = π(π₯4 β 7π₯3 + 6π₯2 + 28π₯ β 40), where π < 0. (π β β 151 if the scales are equal; otherwise one canβt tell how large π is.) 24. There are only two functions, β and π, which can be put in the form π¦ = πΆππ₯ , where πΆ and π are constants: π(π₯) =
π3 ππ₯ = (π3 βπ)ππ₯ , π
where πΆ = π3 βπ since π, π are constants.
1 β(π₯) = β π₯β2 = β5β(π₯β2) = β5βπ₯+2 = (β25)5βπ₯ . 5 Thus, β and π are the only exponential functions.
1.6 SOLUTIONS
69
25. There is only one function, π, who can be put in the form π¦ = π΄π₯2 + π΅π₯ + πΆ: β β β π(π₯) = βπ₯ + π β ππ₯4 = β π π₯2 β π₯ + π, where π΄ = β π, since π is a constant. Thus, π is the only quadratic function. 26. There is only one function, π, which is linear. Function π is a constant linear function whose vertical intercept is the constant ππ2 βπ, since π, π and π are constants. 27. Since π and π are constants, so is πβπ, so π (π₯), which can be rewritten as π (π₯) =
π π₯ + π, π
is a polynomial function. Also, π (π₯) is a rational function since it can be written as a quotient of polynomials with numerator π (π₯) and denominator 1. On the other hand, π (π₯) is not a power function since it is the sum of two terms with diο¬erent powers of π₯, and as there are no terms with π₯ as an exponent, it cannot be an exponential function. Thus, π (π₯) falls into families (III), and (IV). 28. By combining the two terms of π(π₯) over a common denominator, π(π₯) can be rewritten as π(π₯) = ππ₯2 +
π ππ₯4 π ππ₯4 + π = 2 + 2 = . 2 π₯ π₯ π₯ π₯2
Therefore, since π(π₯) can be written as a quotient of polynomials, it is a rational function. However, π(π₯) is not a power function since it is the sum of two terms with diο¬erent 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, π(π₯) falls into family (IV) only. 29. Since π and π are constants, so is πβπ π . In addition, since π is a positive integer, β(π₯), which can be rewritten as ( )π π π₯ β(π₯) = π = π π₯π , π π 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(π₯) is not an exponential function. Thus, β(π₯) falls into families (II), (III) and (IV). 30. Since π is constant, π(π₯) is a power function. Since π 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 ππ₯π 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 and π are constants, so is π + π, so π(π₯), which can be written in the form π(π₯) = ππ₯β1 +
π = ππ₯β1 + ππ₯β1 = (π + π)π₯β1 , π₯
is a power function. We can also write π(π₯) as π(π₯) = (π + π)π₯β1 =
π+π , π₯
a quotient of polynomials, so it is also a rational function. The function π(π₯) is not a polynomial as there are terms with negative powers of π₯, and π(π₯) is not exponential since there are no terms with π₯ as an exponent. Thus, π(π₯) falls into families (II), and (IV). 32. Since π, π, and π are all constants, so is ((π + π)βπ)2 , so π(π₯), which can be written in the form (( ) ) )π₯ ( π+π 2 π + π 2π₯ = , π(π₯) = π π 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, π(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 diο¬erent degrees.
70
Chapter One /SOLUTIONS
34. III and VI, since expanding gives
π¦ = π₯4 β 2π₯2 + 1
and
π¦ = π₯4 β 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: π¦=
π₯2 β 1 . π₯
Since in each case, the denominator is not a constant, these functions cannot be thought of as polynomials. β 36. I, since the numerator has two zeros, π₯ = Β± 2. III, since the polynomial factors to π¦ = β(π₯ β 1)2 (π₯ + 1)2 , it has two zeros, π₯ = Β±1. π₯2 β 1 V, since we can combine terms, π¦ = , and the numerator has two zeros, π₯ = Β±1. π₯ β 2 2 VI, since π¦ = (π₯ β 2)(π₯ + 2) has two distinct zeros, π₯ = Β± 2, from the ο¬rst 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 π¦ = π₯(π₯ β 1)(π₯ + 1).
β 39. II, since the denominator has two zeros, π₯ = Β± 2. 40. I and II, since in each case as π₯ β β or π₯ β ββ, we have π¦βπ¦=
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₯ β 2) 1 π₯β3+π₯β1 2π₯ β 4 1 + = = = π₯β1 π₯β3 (π₯ β 1)(π₯ β 3) (π₯ β 1)(π₯ β 3) (π₯ β 1)(π₯ β 3) Thus, Zeros: π₯ = 2 Asymptotes: π₯ = 1, π₯ = 3. 45. Since the graph of this function is only deο¬ned 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 diο¬erent 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 +β and π₯ β ββ. The ends of a degree 5 polynomial are in Quadrants I and III if the leading coeο¬cient is positive or in Quadrants II and IV if the leading coeο¬cient 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 ο¬ve 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, π , π and π₯3 are graphed in four windows. In the largest of the four windows the graphs are indistinguishable, as required. Answers may vary. π¦
π¦
106
109
β100
100
π₯
β1000
β106
1000
β109 π¦
π¦
1012
β104
π₯
1015
104
π₯
β105
β1012
105
π₯
β1015
Figure 1.74 51. The function is a cubic polynomial with positive leading coeο¬cient. Since the ο¬gure 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 +β as π₯ β +β because the leading coeο¬cient is positive. Therefore, there are exactly three zeros. Two zeros are shown, and occur at approximately π₯ = β1 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(1)2 + π(1) + π = π + π + π. (ii) If (1, 1) is the vertex, then the axis of symmetry is π₯ = 1, so β
π = 1, 2π
and thus
π π = β , so π = β2π. 2 But to be the vertex, (1, 1) must also be on the graph, so we know that π + π + π = 1. Substituting π = β2π, we get βπ + π = 1, which we can rewrite as π = π β 1, or π = 1 + π. (iii) For (0, 6) to be on the graph, we must have π (0) = 6. But π (0) = π(02 ) + π(0) + π = π, so π = 6. (b) To satisfy all the conditions, we must ο¬rst, from (a)(iii), have π = 6. From (a)(ii), π = π β 1 so π = 5. Also from (a)(ii), π = β2π, so π = β10. Thus the completed equation is π¦ = π (π₯) = 5π₯2 β 10π₯ + 6, which satisο¬es all the given conditions. 53. Let us represent the height by β. Since the volume is π , we have π₯2 β = π . Solving for β gives
π . π₯2 The graph is in Figure 1.76. We are assuming π is a positive constant. β=
β
β = π βπ₯2 π₯
Figure 1.76
54. (a) Let the height of the can be β. Then
π = ππ2 β.
The surface area consists of the area of the ends (each is ππ2 ) and the curved sides (area 2ππβ), so π = 2ππ2 + 2ππβ. Solving for β from the formula for π , we have β= Substituting into the formula for π, we get π = 2ππ2 + 2ππ β
π . ππ2 π 2π = 2ππ2 + . π ππ2
(b) For large π, the 2π βπ term becomes negligible, meaning π β 2ππ2 , and thus π β β as π β β.
1.6 SOLUTIONS
73
(c) The graph is in Figure 1.77. π 100 75 π = 2ππ2 + 2ππ π = 10
50 25 0
1
2
3
4
5
π
Figure 1.77 55. Substituting π€ = 65 and β = 160, we have (a)
π = 0.01(650.25 )(1600.75 ) = 1.3 m2 .
(b) We substitute π = 1.5 and β = 180 and solve for π€: 1.5 = 0.01π€0.25 (1800.75 ). We have
1.5 = 3.05. 0.01(1800.75 ) Since π€0.25 = π€1β4 , we take the fourth power of both sides, giving π€0.25 =
π€ = 86.8 kg. (c) We substitute π€ = 70 and solve for β in terms of π : π = 0.01(700.25 )β0.75 , so
π . 0.01(700.25 ) Since β0.75 = β3β4 , we take the 4β3 power of each side, giving )4β3 ( π π 4β3 β= = 0.01(700.25 ) (0.014β3 )(701β3 ) β0.75 =
so
β = 112.6π 4β3 .
56. Let π·(π£) 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 π·(π£) = ππ£2 where π is a constant of proportionality. To determine the value of π, we use the fact that π·(70) = 148. π·(70) = π(70)2 = 148. Thus,
148 β 0.0302. 702 ) ( 148 148 = 37 ft (35)2 = π·(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 ο¬gured it out that way, without solving for π explicitly.) π·(140) =
(
74
Chapter One /SOLUTIONS
57. (a) Since the rate π varies directly with the fourth power of the radius π, we have the formula π = ππ4 where π is a constant. (b) Given π = 400 for π = 3, we can determine the constant π. 400 = π(3)4 400 = π(81) 400 β 4.93827. π= 81 So the formula is
π = 4.93827π4
(c) Evaluating the formula above at π = 5 yields π = 4.93827(5)4 = 3086.42
cm3 . sec
58. The pomegranate is at ground level when π (π‘) = β16π‘2 + 64π‘ = β16π‘(π‘ β 4) = 0, so when π‘ = 0 or π‘ = 4. At time π‘ = 0 it is thrown, so it must hit the ground at π‘ = 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 π (π‘) = β16π‘2 + 64π‘ = β16(π‘ β 2)2 + 64, which is a downward parabola with vertex (i.e., highest point) at (2, 64). The maximum height is π (2) = 64 feet. 59. (a) The object starts at π‘ = 0, when π = π£0 (0) β π(0)2 β2 = 0. Thus it starts on the ground, with zero height. (b) The object hits the ground when π = 0. This is satisο¬ed at π‘ = 0, before it has left the ground, and at some later time π‘ that we must solve for. ( ) 0 = π£0 π‘ β ππ‘2 β2 = π‘ π£0 β ππ‘β2 Thus π = 0 when π‘ = 0 and when π£0 β ππ‘β2 = 0, i.e., when π‘ = 2π£0 βπ. The starting time is π‘ = 0, so it must hit the ground at time π‘ = 2π£0 βπ. (c) The object reaches its maximum height halfway between when it is released and when it hits the ground, or at π‘ = (2π£0 βπ)β2 = π£0 βπ. (d) Since we know the time at which the object reaches its maximum height, to ο¬nd the height it actually reaches we just use the given formula, which tells us π at any given π‘. Substituting π‘ = π£0 βπ, ( ) ( ) π£20 π£20 π£20 π£0 1 = β π β π = π£0 π 2 π 2π π2 =
2π£20 β π£20 2π
=
π£20 2π
.
60. (a) π (π ) = ππ (πΏ β π ), where π is a positive constant. (b) A possible graph is in Figure 1.78. π
πΏ
Figure 1.78
π
1.6 SOLUTIONS
75
61. Yes. The graph of this power function is increasing and concave down for positive mass π. 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. πΏ πΏ = 2π 1β4
π
Figure 1.79 62. No. The graph of this polynomial function is increasing but concave up for positive mass π. 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. πΏ
πΏ = 0.2π 3 + π 4 π
Figure 1.80 63. No. The graph of this power function is decreasing for positive mass π. 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. πΏ
πΏ = 2π β1β4
π
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. πΏ πΏ=
4(π + 1)2 β 4 (π + 1)2
π
Figure 1.82
76
Chapter One /SOLUTIONS
65. No. The graph of this rational function is decreasing for positive mass π. 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. πΏ
πΏ=
10(π + 1)2 β 1 (π + 1)3 π
Figure 1.83
66. To ο¬nd the horizontal asymptote, we look at end behavior. As π₯ β Β±β, the lower-degree terms of π (π₯) become insignificant, and π (π₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π₯ β Β±β, we see that 5 5π₯ = . π (π₯) β 2π₯ 2 There is a horizontal asymptote at π¦ = 5β2. To ο¬nd the vertical asymptotes, we set the denominator equal to zero. When 2π₯ + 3 = 0, we have π₯ = β3β2 so there is a vertical asymptote at π₯ = β3β2. 67. To ο¬nd the horizontal asymptote, we look at end behavior. As π₯ β Β±β, the lower-degree terms of π (π₯) become insignificant, and π (π₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π₯ β Β±β, we see that π₯2 π (π₯) β 2 = 1. π₯ There is a horizontal asymptote at π¦ = 1. To ο¬nd the vertical asymptotes, we set the denominator equal to zero. When π₯2 β 4 = 0, we have π₯ = Β±2 so there are vertical asymptotes at π₯ = β2 and at π₯ = 2. 68. To ο¬nd the horizontal asymptote, we look at end behavior. As π₯ β Β±β, the lower-degree terms of π (π₯) become insignificant, and π (π₯) becomes approximated by the highest degree term of the numerator and denominator. Thus, as π₯ β Β±β, we see that 5π₯3 π (π₯) β 3 = 5. π₯ There is a horizontal asymptote at π¦ = 5. To ο¬nd the vertical asymptotes, we set the denominator equal to zero. When π₯3 β 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 β5π₯4 globally. Thus we have: π (π₯) β ββ as π₯ β ββ, and π (π₯) β ββ as π₯ β +β. (b) Polynomials behave globally as their leading term, so this rational function behaves globally as (3π₯2 )β(2π₯2 ), or 3β2. Thus we have: π (π₯) β 3β2 as π₯ β ββ, and π (π₯) β 3β2 as π₯ β +β. (c) We see from a graph of π¦ = ππ₯ that π (π₯) β 0 as π₯ β ββ, and π (π₯) β +β as π₯ β +β. 70. π(π₯) = 2π₯2 , β(π₯) = π₯2 + π for any π > 0. Notice that the graph is symmetric about the π¦-axis and limπ₯ββ π (π₯) = 2. 71. We use the fact that at a constant speed, Time = DistanceβSpeed. Thus, Total time = Time running + Time walking 3 6 = + . π₯ π₯β2 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 coeο¬cient = 1. Therefore, π₯2 π¦ β 2 = 1 as π₯ β Β±β. π₯ (b) I, since π₯ π¦ β 2 = 0 as π₯ β Β±β. π₯ (c) II and III, since replacing π₯ by βπ₯ leaves the graph of the function unchanged. (d) None (e) III, since the denominator is zero and π (π₯) tends to Β±β when π₯ = Β±1. 73. β(π‘) cannot be of the form ππ‘2 or ππ‘3 since β(0.0) = 2.04. Therefore β(π‘) must be the exponential, and we see that the ratio of successive values of β is approximately 1.5. Therefore β(π‘) = 2.04(1.5)π‘ . If π(π‘) = ππ‘2 , then π = 3 since π(1.0) = 3.00. However, π(2.0) = 24.00 β 3 β 22 . Therefore π(π‘) = ππ‘3 , and using π(1.0) = 3.00, we obtain π(π‘) = 3π‘3 . Thus π (π‘) = ππ‘2 , and since π (2.0) = 4.40, we have π (π‘) = 1.1π‘2 . 74. The graphs are shown in Figure 1.84. π¦
(a) 9
π¦
(b) π₯4
3π₯
50000
π₯4
3π₯
5
π¦
(c)
625
π₯
5
3π₯
π₯4 π₯
10
π₯
Figure 1.84 75. Since the parabola opens upward, we must have π > 0. To determine a relationship between π₯ and π¦ at the point of intersection π , we eliminate π from the parabola and circle equations. Since π¦ = π₯2 βπ, we have π = π₯2 βπ¦. Putting this into the circle equation gives π₯2 + π¦2 = 2π₯4 βπ¦2 . Rewrite this as π₯2 π¦2 + π¦4 = 2π₯4 π¦4 + π₯2 π¦2 β 2π₯4 = 0 2
(π¦ + 2π₯2 )(π¦2 β π₯2 ) = 0. This means π₯2 = π¦2 (since π¦2 cannot equal β2π₯2 ). Thus π₯ = π¦ since π is in the ο¬rst quadrant. So π moves out along the line π¦ = 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 undeο¬ned. This happens when π£2 = 0, or at π£2 = π 2 . π2 Since π£ > 0, the graph of the exact formula has a vertical asymptote where 1β
π£ = π = 3 β 108 m/sec. πΈ (1017 joules)
(
5
πΈ = ππ 2
4
1 β β1 1βπ£2 βπ 2
3 2
πΈ = 12 ππ£2
1 1
2
3
4
5
Figure 1.85
π£ (108 m/sec)
)
78
Chapter One /SOLUTIONS (b) The ο¬rst formula does not give a good approximation to the exact formula when the graphs are not close together. This happens for π£ > 1.5 β 108 m/sec. For π£ < 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 π£-axis that a more careful analysis should be made. We should zoom in and redraw the graph.
77. Since π§ = ln π₯, we have π₯ = ππ§ . Hence π¦ = 100π₯β0.2 = 100(ππ§ )β0.2 = 100πβ0.2π§ .
Strengthen Your Understanding 78. The graph of a polynomial of degree 5 cuts the horizontal axis at most ο¬ve times, but it could be fewer. For example, π (π₯) = π₯5 cuts the π₯-axis only once. 79. A fourth degree polynomial tends to negative inο¬nity if the leading coeο¬cient (coeο¬cient of the π₯4 term) is negative. For example, π (π₯) = βπ₯4 tends to negative inο¬nity as π₯ β β. 80. A rational function has no vertical asymptotes if the denominator has no zeros. For example: π (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. π¦ π¦ = π₯5
3
π¦ = π₯3
2 1 0.5
1
1.5
π₯
Figure 1.86
82. The rational function π (π₯) = (π₯3 + 1)βπ₯ has no horizontal asymptotes. To see this, observe that π¦ = π (π₯) =
π₯3 π₯3 + 1 β = π₯2 π₯ π₯
for large π₯. Thus, π¦ β β as π₯ β Β±β. 83. Let π (π₯) = π₯β(π₯2 + 1). Since
π₯ 1 π₯ β 2 = for large π₯, π₯ π₯2 + 1 π₯ and 1βπ₯ β 0 as π₯ β β, the function π (π₯) has horizontal asymptote π¦ = 0. We have π (0) = 0, so π (π₯) crosses this asymptote at π₯ = 0. π¦=
84. One possibility is π(π₯) = (π₯ β 1)(π₯ β 2)(π₯ β 3) = π₯3 β 6π₯2 + 11π₯ β 6. 85. A possible function is π (π₯) =
3π₯ . π₯ β 10
π (π₯) =
1 . π₯2 + 1
86. One possibility is
1.6 SOLUTIONS
79
1 . Other answers are possible. π₯ + 7π 1 . This function has an asymptote corresponding to every factor in 88. Let π (π₯) = (π₯ β 1)(π₯ β 2)(π₯ β 3) β― (π₯ β 16)(π₯ β 17) the denominator. Other answers are possible. π₯β1 89. The function π (π₯) = has π¦ = 1 as the horizontal asymptote and π₯ = 2 as the vertical asymptote. These lines cross π₯β2 at the point (2, 1). Other answers are possible.
87. Let π (π₯) =
90. False. The polynomial π (π₯) = π₯2 + 1, with degree 2, has no real zeros. 91. True. If the degree of the polynomial, π(π₯), is π, then the leading term is ππ π₯π with ππ β 0. If π is odd and ππ is positive, π(π₯) tends toward β as π₯ β β and π(π₯) tends toward ββ as π₯ β ββ. Since the graph of π(π₯) has no breaks in it, the graph must cross the π₯-axis at least once. If π is odd and ππ is negative, a similar argument applies, with the signs reversed, but leading to the same conclusion. 92. False. Suppose π (π₯) = π(π₯) = π₯2 . Then the composition is quartic (fourth degree), not quadratic: π (π(π₯)) = π (π₯2 ) = (π₯2 )2 = π₯4 . 93. True. If we factor and simplify the rational expression, we see that π (π₯) =
5π₯(π₯ + 1)(π₯ β 1) = 5π₯ β 5, for π₯ β β1, 0. π₯(π₯ + 1)
Hence, over π₯ > 0 the graph of the π is the same at the graph of the linear function π¦ = 5π₯ β 5. 94. (a), (c), (d), (e), (b). Notice that π (π₯) and β(π₯) are decreasing functions, with π (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 π (π₯ + 2) β π (π₯) = π + π(π₯ + 2) β (π + ππ₯) = 2π. The diο¬erence is constant, because it does not depend on π₯. (b) (III) For exponential functions we have π (π₯ + 2) πππ(π₯+2) = π (π₯) ππππ₯ ππππ₯ π2π = = π2π . ππππ₯ The quotient is constant, because it does not depend on π₯. (c) (IV) For power functions we have π (2π₯) π(2π₯)π = π (π₯) ππ₯π π2π π₯π = = 2π . ππ₯π The quotient is constant, because it does not depend on π₯. (d) (II) For logarithmic functions we have π (2π₯) β π (π₯) = (π + π ln(2π₯)) β (π + π ln π₯) = (π + π ln 2 + π ln π₯) β (π + π ln π₯) = π ln 2. The diο¬erence is constant, because it does not depend on π₯.
80
Chapter One /SOLUTIONS
96. Properties of logs give
ln(ππ₯π ) = ln π + ln π₯π = ln π + π ln π₯.
Therefore π
π
ln(ππ₯2 ) β ln(ππ₯1 ) ln π (π₯2 ) β ln π (π₯1 ) = ln π₯2 β ln π₯1 ln π₯2 β ln π₯1 ln π + π ln π₯2 β ln π β π ln π₯1 = ln π₯2 β ln π₯1 π(ln π₯2 β ln π₯1 ) = = π. ln π₯2 β ln π₯1
Solutions for Section 1.7 EXERCISES 1. (a) The function π has jumps in the graph at π₯ = β1 and at π₯ = 1. Therefore, π is not continuous at π₯ = β1 and at π₯ = 1. (b) The domain of π is β3 β€ π₯ β€ 3, and by part (a), we know that π is not continuous at π₯ = β1 and at π₯ = 1. Therefore, π is continuous on β3 < π₯ < β1, β1 < π₯ < 1, and 1 < π₯ < 3. 2. (a) The function π has a break in the graph at π₯ = 1 and jumps in the graph at π₯ = 2 and at π₯ = 4. Therefore, π is not continuous at π₯ = 1, 2, and 4. (b) The domain of π is 0 β€ π₯ β€ 6, and by part (a), we know that π is not continuous at π₯ = 1, 2 and at 4. Therefore, π is continuous on 0 < π₯ < 1, 1 < π₯ < 2, 2 < π₯ < 4, and 4 < π₯ < 6. 3. (a) As π₯ approaches β3 from either side, the values of π (π₯) get closer and closer to 1, so the limit appears to be about 1. (b) As π₯ approaches β2 from either side, the values of π (π₯) get closer and closer to 2, so the limit appears to be about 2. (c) As π₯ approaches β1, the values of π (π₯) get closer and closer to 3 on one side of π₯ = β1 and get closer and closer to 2 on the other side of π₯ = β1. Thus the limit does not exist. (d) As π₯ approaches 0 from either side, the values of π (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 π (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 π (π₯) get closer and closer to 2. (Recall that to ο¬nd 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₯ = β1, π (π₯) is not continuous at π₯ = β1. Since the graph has a hole at π₯ = 2, π (π₯) is not continuous at π₯ = 2. (b) As π₯ approaches β1 from either side, the values of π (π₯) get closer and closer to 2 on one side of π₯ = β1 and get closer and closer to 5 on the other side of π₯ = β1. Thus lim π (π₯) does not exist. As π₯ approaches 2 from either side, π₯ββ1
the values of π (π₯) get closer and closer to β3, so the limit appears to be about β3. 5. (a) Since the graph has a hole at π₯ = β2, π (π₯) is not continuous at π₯ = β2. Since the graph has an asymptote at π₯ = 3, π (π₯) is not continuous at π₯ = 3. (b) As π₯ approaches β2 from either side, the values of π (π₯) get closer and closer to β3, so the limit appears to be about β3. As π₯ approaches 3 from either side, the values of π (π₯) approach β. Thus lim π (π₯) does not exist. π₯β3
6. Values of π (π₯) appear to approach 2 as π₯ gets close to 0 from both sides, so lim π (π₯) appears to be 2. π₯β0
We do not know for sure the limit is 2 because for values of π₯ close to 0 diο¬erent from those in the table, the values of π (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 π(π‘) appear to approach 1 as π‘ gets close to 3 from both sides, so lim π(π‘) appears to be 1. π‘β3
We do not know for sure the limit is 1 because for values of π‘ close to 3 diο¬erent from those in the table, the values of π(π‘) 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 π (π₯) gives: π₯
β0.1
β0.01
0.01
0.1
π (π₯)
4.794
4.998
4.998
4.794
1.7 SOLUTIONS
81
(b) Since the values of π (π₯) appear to get closer and closer to 5 as π₯ gets closer and closer to 0, we estimate lim π₯β0
sin(5π₯) = 5. π₯
sin(5π₯) is undeο¬ned at π₯ = 0. π₯ 9. (a) Substituting π₯-values into π (π₯) gives: Notice that π (π₯) =
π₯
β0.1
β0.01
0.01
0.1
π (π₯)
2.592
2.955
3.045
3.499
(b) Since the values of π (π₯) appear to get closer and closer to 3 as π₯ gets closer and closer to 0, we estimate lim π₯β0
π3π₯ β 1 = 3. π₯
π3π₯ β 1 is undeο¬ned at π₯ = 0. π₯ 10. We evaluate π (π₯) = 5 + ln π₯ for values of π₯ closer and closer to 1. Notice that π (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 π (π₯) gets closer and closer to 5, so we estimate lim(5 + ln π₯) = 5. π₯β1
11. Yes, because π₯ β 2 is not zero on this interval. 12. No, because π₯ β 2 = 0 at π₯ = 2. 13. Yes, because 2π₯ β 5 is positive for 3 β€ π₯ β€ 4. 14. No, because 2π₯ + π₯β1 is undeο¬ned at π₯ = 0. 15. No, because cos(πβ2) = 0. 16. Yes, because cos π is not zero on this interval. 17. (a) At π₯ = 1, on the line π¦ = π₯, we have π¦ = 1. At π₯ = 1, on the parabola π¦ = π₯2 , we have π¦ = 1. Thus, π (π₯) is continuous. See Figure 1.87. (b) At π₯ = 3, on the line π¦ = π₯, we have π¦ = 3. At π₯ = 3, on the parabola π¦ = π₯2 , we have π¦ = 9. Thus, π(π₯) is not continuous. See Figure 1.88. π¦
π¦
π(π₯)
π (π₯)
1
Figure 1.87
π₯
3
π₯
Figure 1.88
18. (a) Since the graph of π is comprised of portions of either linear or quadratic functions, π is continuous everywhere except possibly at π₯ = 3 and π₯ = 5, where the formula for the function π changes. Since the graph of 4 β π₯ goes through the point (3, 1) but the graph of π₯2 β 8π₯ + 17 goes through the point (3, 2), there is a jump in the graph of π at π₯ = 3, meaning that π is not continuous at π₯ = 3. On the other hand, the graph of π₯2 β 8π₯ + 17 and 12 β 2π₯ both go through the point (5, 2), so π is continuous at π₯ = 5. Thus, π₯ = 3 is the only value of π₯ at which π is not continuous. (b) By part (a), we know that π is not continuous at π₯ = 3. Therefore, π is continuous on 0 < π₯ < 3 and 3 < π₯ < 6.
82
Chapter One /SOLUTIONS
19. We have that π (0) = β1 < 0 and π (1) = 1 > 0 and that π is continuous. Thus, by the Intermediate Value Theorem applied to π = 0, there is a number π in [0, 1] such that π (π) = π = 0. 20. We have that π (0) = 1 > 0 and π (1) = π β 3 < 0 and that π is continuous. Thus, by the Intermediate Value Theorem applied to π = 0, there is a number π in [0, 1] such that π (π) = π = 0. 21. We have that π (0) = β1 < 0 and π (1) = 1 β cos 1 > 0 and that π is continuous. Thus, by the Intermediate Value Theorem applied to π = 0, there is a number π in [0, 1] such that π (π) = π = 0. 22. Since π is not continuous at π₯ = 0, we consider instead the smaller interval [0.01, 1]. We have that π (0.01) = 20.01 β100 < 0 and π (1) = 2 β 1β1 = 1 > 0 and that π is continuous. Thus, by the Intermediate Value Theorem applied to π = 0, there is a number π in [0.01, 1], and hence in [0, 1], such that π (π) = π = 0. π₯2 β 4 at π₯ = 2 gives us 0β0, so we see if we can rewrite the function using algebra. We have 23. Evaluating π₯β2 (π₯ + 2)(π₯ β 2) π₯2 β 4 = . π₯β2 π₯β2 Since π₯ β 2 in the limit, we can cancel the common factor π₯ β 2 to see lim π₯β2
24. Evaluating
(π₯ + 2)(π₯ β 2) π₯2 β 4 = lim = lim(π₯ + 2) = 4. π₯β2 π₯β2 π₯β2 π₯β2
π₯2 β 9 at π₯ = β3 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯+3 (π₯ + 3)(π₯ β 3) π₯2 β 9 = . π₯+3 π₯+3
Since π₯ β β3 in the limit, we can cancel the common factor π₯ + 3 to see lim
π₯ββ3
25. Evaluating
(π₯ + 3)(π₯ β 3) π₯2 β 9 = lim = lim (π₯ β 3) = β6. π₯ββ3 π₯ββ3 π₯+3 π₯+3
π₯2 + 4π₯ β 5 at π₯ = 1 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯β1 (π₯ + 5)(π₯ β 1) π₯2 + 4π₯ β 5 = . π₯β1 π₯β1
Since π₯ β 1 in the limit, we can cancel the common factor π₯ β 1 to see lim π₯β1
26. Evaluating
(π₯ + 5)(π₯ β 1) π₯2 + 4π₯ β 5 = lim = lim(π₯ + 5) = 6. π₯β1 π₯β1 π₯β1 π₯β1
π₯2 β 4π₯ + 3 at π₯ = 1 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯2 + 3π₯ β 4 (π₯ β 1)(π₯ β 3) π₯2 β 4π₯ + 3 = . (π₯ + 4)(π₯ β 1) π₯2 + 3π₯ β 4
Since π₯ β 1 in the limit, we can cancel the common factor π₯ β 1 to see lim
π₯2 β 4π₯ + 3
π₯β1 π₯2 + 3π₯ β 4
= lim
(π₯ β 1)(π₯ β 3)
π₯β1 (π₯ + 4)(π₯ β 1)
= lim
π₯β3
π₯β1 π₯ + 4
=
β2 . 5
π₯2 + 4 is continuous everywhere on its domain (that is, at every point except π₯ = β8.) In particular, it is π₯+8 continuous at π₯ = 1 so we ο¬nd the limit by evaluating the expression at π₯ = 1. We have
27. The expression
5 π₯2 + 4 = . π₯β1 π₯ + 8 9
lim
1.7 SOLUTIONS
83
28. Evaluating the expression at β = 0, we arrive at 0β0. Rewriting the expression using algebra gives lim
ββ0
(5 + β)2 β 52 (25 + 10β + β2 ) β 25 = lim ββ0 β β 10β + β2 = lim ββ0 β β(10 + β) = lim ββ0 β and since β β 0, canceling the common factor of β, we have = lim(10 + β) ββ0
= 10.
29. Since ππ₯ + 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₯ β π)β(π₯2 + π₯) is continuous at π₯ = 2, the limit can be found by substituting π₯ = 2. Thus, (2 + 6)(2 β π) =4 22 + 2 π = β1. 31. The value of π¦ on the line π¦ = ππ₯ at π₯ = 3 is π¦ = 3π. To make π (π₯) continuous, we need 3π = 5
so
π=
5 . 3
See Figure 1.89. π¦
π (π₯)
5
6 π¦=5
I
π¦ = (5β3)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 ππ₯ 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 ππ₯ goes through the point (1, 4). Thus π = 4. 34. If the graphs of π¦ = π‘ + π and π¦ = ππ‘ meet at π‘ = 5, we have 5 + π = 5π π = 5β4. See Figure 1.90.
84
Chapter One /SOLUTIONS π¦ π¦ = (5β4)π‘ π(π‘) π¦ = (5β4) + π‘
5 4
5
10
π‘
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 π (π‘) is graphed in Figure 1.91. 12
6
time (seconds)
7
Figure 1.91: Voltage change from 6V to 12V Using formulas, the voltage, π (π‘), is represented by { π (π‘) =
6,
0<π‘β€7
12,
7<π‘
Although a real physical voltage is continuous, the voltage in this circuit is well-approximated by the function π (π‘), which is not continuous on any interval around 7 seconds. 37. (a) The function π has a jump in the graph at π‘ = 5 so it is not continuous. The discontinuity at π‘ = 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 cliο¬ and its height decreases over time until π‘ = 5 when it hits the ground. For 5 β€ π‘ β€ 7, we have β = 0 since the stone is on the ground. Therefore Figure 1.92 is a possible graph. The function π is continuous because there is no sudden change in the height of the stone. β
π(π‘)
5
Figure 1.92
7
π‘
1.7 SOLUTIONS
85
38. (a) For 0 β€ π‘ β€ 2, the car is accelerating, so π is increasing. For 2 β€ π‘ β€ 3, the speed of the car is constant, so π is constant. Finally, at π‘ = 3, the speed of the car drops to zero when it hits the barrier. A possible graph of π is shown in Figure 1.93. π£
1
2
3
4
π‘
Figure 1.93 (b) No, π is not continuous because the speed of the car suddenly drops when it hits the barrier, resulting in a jump in the graph of π at π‘ = 3 seconds. 39. The graph of π suggests that π is not continuous on any interval containing π = 0, since π(0) = 1β2. 40. For π₯ > 0, we have |π₯| = π₯, so π (π₯) = 1. For π₯ < 0, we have |π₯| = βπ₯, so π (π₯) = β1. Thus, the function is given by { 1 π₯>0 π (π₯) = 0 π₯=0 β1 π₯ < 0 , so π 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₯β0 π₯ 1
|π₯| π₯
β1
1
π₯
β1
Figure 1.94 42. For β1 β€ π₯ β€ 1, β 1 β€ π¦ β€ 1, the graph of π¦ = π₯ ln |π₯| is in Figure 1.95. The graph suggests that lim π₯ ln |π₯| = 0. π₯β0
π¦ 1 π¦ = π₯ ln |π₯|
β1
1
β1
Figure 1.95
π₯
86
Chapter One /SOLUTIONS
43. For β0.5 β€ π β€ 0.5, 0 β€ π¦ β€ 3, the graph of π¦ =
sin (2π) is shown in Figure 1.96. The graph suggests that π sin (2π) lim = 2. πβ0 π π¦
π¦ = sin(2π) π
0
0.5
2 1
β0.5
π
Figure 1.96 sin π 44. For β90β¦ β€ π β€ 90β¦ , 0 β€ π¦ β€ 0.02, the graph of π¦ = is shown in Figure 1.97. By tracing along the curve, we see π that in degrees, sin π = 0.01745 β¦ . lim πβ0 π sin π π
0.02 0.01
β90
0
90
π (degree)
Figure 1.97
45. A graph of π¦ = estimate that
πβ β 1 in a window such as β0.5 β€ β β€ 0.5 and 0 β€ π¦ β€ 3 appears to indicate π¦ β 1 as β β 0. We β πβ β 1 = 1. ββ0 β lim
46. A graph of π¦ = estimate that
π5β β 1 in a window such as β0.5 β€ β β€ 0.5 and 0 β€ π¦ β€ 6 appears to indicate π¦ β 5 as β β 0. We β lim
ββ0
π5β β 1 = 5. β
2β β 1 47. A graph of π¦ = in a window such as β0.5 β€ β β€ 0.5 and 0 β€ π¦ β€ 1 appears to indicate π¦ β 0.7 as β β 0. By β zooming in on the graph, we can estimate the limit more accurately. Therefore, we estimate that lim
ββ0
2β β 1 = 0.693. β
cos(3β) β 1 in a window such as β0.5 β€ β β€ 0.5 and β1 β€ π¦ β€ 1 appears to indicate π¦ β 0 as β β 0. 48. A graph of π¦ = β Therefore, we estimate that cos(3β) β 1 = 0. lim ββ0 β
1.7 SOLUTIONS
87
49. Let π (π₯) = (2π₯2 β 32)β(π₯ + 4). We can estimate the limit of π (π₯) as π₯ goes to 4 by putting in π₯-values closer and closer to π₯ = 4. In Table 1.8 the values of π (π₯) appear to get closer and closer to 0 as π₯ gets closer to 4, so we estimate 2π₯2 β 32 = 0. π₯β4 π₯+4
lim
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.98 suggests that lim π₯β4
2π₯2 β 32 = 0. π₯+4
Since π (π₯) is continuous at π₯ = 4, we can also ο¬nd the limit exactly by substituting π₯ = 4. This gives 2 β 42 β 32 2π₯2 β 32 = = 0. π₯β4 π₯+4 4+4
lim Table 1.8 π₯
3.9
3.99
3.999
4.001
4.01
4.1
π (π₯)
β0.2
β0.02
β0.002
0.002
0.02
0.2
1 0.5 0
3.5
β0.5
4
4.5
5
π₯
β1
Figure 1.98 50. Let π (π₯) = (2π₯2 β 32)β(π₯ + 4). We can estimate the limit of π (π₯) as π₯ goes to β4 by putting in π₯-values closer and closer to π₯ = β4. In Table 1.9, the values of π (π₯) appear to get closer and closer to β16 as π₯ gets closer to β4, so we estimate lim
π₯ββ4
2π₯2 β 32 = β16. π₯+4
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.99 suggests that 2π₯2 β 32 = β16. π₯ββ4 π₯ + 4 lim
We can also use algebra to ο¬nd the limit exactly. We have 2(π₯ + 4)(π₯ β 4) 2π₯2 β 32 = . π₯+4 π₯+4 Since π₯ β β4 in the limit, we can cancel the common factor π₯ + 4 to see 2(π₯ + 4)(π₯ β 4) 2π₯2 β 32 = lim = lim 2(π₯ β 4) = β16. π₯ββ4 π₯ + 4 π₯ββ4 π₯ββ4 π₯+4 lim
Table 1.9 π₯
β4.1
β4.01
β4.001
β3.999
β3.99
β3.9
π (π₯)
β16.2
β16.02
β16.002
β15.998
β15.98
β15.8
β5
β4.5
β4
β3.5
π₯ β15
(β4, β16)
β16 β17 β18
Figure 1.99
88
Chapter One /SOLUTIONS
51. Let π (π₯) = (3π₯ β 1)β(sin π₯). We can estimate the limit of π (π₯) as π₯ goes to 0 by putting in π₯-values closer and closer to π₯ = 0. In Table 1.10, the values of π (π₯) appear to get closer and closer to 1.099 as π₯ gets closer to 0, so we estimate lim π₯β0
3π₯ β 1 = 1.099. sin π₯
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.100 suggests that lim π₯β0
3π₯ β 1 = 1.099. sin π₯
There are no direct purely algebraic manipulations we can perform to calculate this limit exactly. Table 1.10 π₯
β0.1
β0.01
β0.001
β0.0001
0.0001
0.001
0.01
0.1
π (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 β0.5 β0.25
0
0.25
π₯
0.5
Figure 1.100 β 52. Let π (π₯) = ( π₯ β 2)β(π₯ β 4). We can estimate the limit of π (π₯) as π₯ goes to 4 by putting in π₯-values closer and closer to π₯ = 4. In Table 1.11, the values of π (π₯) appear to get closer and closer to 0.25 as π₯ gets closer to 4, so we estimate β π₯β2 = 0.25. lim π₯β4 π₯ β 4 Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.101 suggests that β π₯β2 lim = 0.25. π₯β4 π₯ β 4 We can also use algebra to ο¬nd the limit exactly. We have β β π₯β2 π₯β2 . = β β π₯β4 ( π₯ β 2)( π₯ + 2) β Since π₯ β 4 in the limit, we can cancel the common factor π₯ β 2 to see β β π₯β2 π₯β2 1 1 = lim β = = 0.25. lim = lim β β π₯β4 π₯ β 4 π₯β4 π₯β4 4 ( π₯ β 2)( π₯ + 2) π₯+2 Table 1.11 π₯
3.9
3.99
3.999
4.001
4.01
4.1
π (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 π (π₯) = (π₯4 β π₯2 )β(π₯ + 1). We can estimate the limit of π (π₯) as π₯ goes to 1 by putting in π₯-values closer and closer to π₯ = β1. In Table 1.12, the values of π (π₯) appear to get closer and closer to β2 as π₯ gets closer to β1, so we estimate π₯ 4 β π₯2 = β2. π₯ββ1 π₯ + 1 lim
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.102 suggests that lim
π₯ββ1
π₯ 4 β π₯2 = β2. π₯+1
We can also use algebra to ο¬nd the limit exactly. We have π₯2 (π₯2 β 1) π₯2 (π₯ β 1)(π₯ + 1) π₯4 β π₯ 2 = = . π₯+1 π₯+1 π₯+1 Since π₯ β β1 in the limit, we can cancel the common factor π₯ + 1 to see π₯2 (π₯ β 1)(π₯ + 1) π₯ 4 β π₯2 = lim = lim π₯2 (π₯ β 1) = β2. π₯ββ1 π₯ + 1 π₯ββ1 π₯ββ1 π₯+1 lim
Table 1.12 π₯
β1.1
β1.01
β1.001
β0.999
β0.99
β0.9
π (π₯)
β2.541
β2.05
β2.005
β1.995
β1.95
β1.539
β1.5
β1
β0.5
2 π₯ β2
(β1 β 2)
β4 β6
Figure 1.102 54. Let π (π₯) = (16 β 8π₯)β(2π₯ β 4). We can estimate the limit of π (π₯) as π₯ goes to 2 by putting in π₯-values closer and closer to π₯ = 2. In Table 1.13, the values of π (π₯) appear to get closer and closer to β2.885 as π₯ gets closer and closer to 2, so we estimate 16 β 8π₯ = β2.885. lim π₯ π₯β2 2 β 4 Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.103 suggests that lim π₯β2
16 β 8π₯ = β2.885. 2π₯ β 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
π (π₯)
β2.987
β2.895
β2.886
β2.885
β2.885
β2.884
β2.875
β2.787
0
1
2
β3
3
π₯
(2, β2.885)
β6
Figure 1.103
90
Chapter One /SOLUTIONS
55. Let π (π₯) = (1 β 3π₯ )β(ππ₯ β 1). We can estimate the limit of π (π₯) as π₯ goes to 0 by putting in π₯-values closer and closer to π₯ = 0. In Table 1.14, the values of π (π₯) appear to get closer and closer to β1.099 as π₯ gets closer to 0, so we estimate 1 β 3π₯ = β1.099. π₯β0 ππ₯ β 1
lim
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.104 suggests that lim
1 β 3π₯
π₯β0 ππ₯ β 1
= β1.099.
There are no direct purely algebraic manipulations we can perform to calculate this limit exactly. Table 1.14 π₯
β0.1
β0.01
β0.001
0.001
0.01
0.1
π (π₯)
β1.093
β1.098
β1.099
β1.099
β1.099
β1.104
β1
β0.5
0.5
π₯
1
β1 (0, β1.099) β2
Figure 1.104 56. Let π (π₯) = (4π₯ β 16)β(2π₯ β 4). We can estimate the limit of π (π₯) as π₯ goes to 2 by putting in π₯-values closer and closer to π₯ = 2. In Table 1.15, the values of π (π₯) appear to get closer and closer to 8 as π₯ gets closer to 2, so we estimate lim π₯β2
4π₯ β 16 = 8. 2π₯ β 4
Alternatively, we can use the graph of π (π₯) to estimate the limit. Figure 1.105 suggests that 4π₯ β 16 = 8. π₯β2 2π₯ β 4
lim
We can also use algebra to ο¬nd the limit exactly. We have (2π₯ )2 β 16 (2π₯ β 4)(2π₯ + 4) 4π₯ β 16 = = . 2π₯ β 4 2π₯ β 4 2π₯ β 4 Since π₯ β 2 in the limit, we can cancel the common factor 2π₯ β 4 to see (2π₯ β 4)(2π₯ + 4) 4π₯ β 16 = lim = lim(2π₯ + 4) = 8. π₯ π₯β2 2 β 4 π₯β2 π₯β2 2π₯ β 4
lim
Table 1.15 π₯
1.9
1.99
1.999
2.001
2.01
2.1
π (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, the curve π¦ = π cos π₯ has π¦ = π cos π = βπ. At π₯ = π, the line π¦ = 12 β π₯ has π¦ = 12 β π. If β(π₯) is continuous, we need βπ = 12 β π π = π β 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 ππ₯ takes the value π β 1 = π at π₯ = 1, we choose π so that the graph of 2ππ₯ + 3 goes through the point (1, π). This gives 2π β 1 + 3 = π π = β3. 59. For any value of π, the function is continuous at every point except π₯ = π. We choose π to make the function continuous at π₯ = π. Since π sin π₯ takes the value π sin π = 0 at π₯ = π, we cannot choose π so that the graph of π₯ + 4 goes through the point (π, 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 πππ₯ goes through the point (2, 3). This gives π2π = 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(ππ₯) 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 = sinβ1 0.5 =
π . 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(ππ₯ + 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 = π6 π6 β 1 π= . 2 63. (a) We see that π (π₯) has jumps at the points π₯ = 1, π₯ = 3, and π₯ = 5. Therefore, π (π₯) is discontinuous at π₯ = 1, 3, and 5. (b) Observe that, on the intervals 0 β€ π₯ < 1 and 3 < π₯ β€ 5, the function π (π₯) is positive, so |π (π₯)| = π (π₯). On the interval 1 β€ π₯ β€ 3, we have |π (π₯)| = | β 2| = 2, and on the interval 5 < π₯ β€ 6, we have |π (π₯)| = | β 3| = 3. Using this information, we sketch the graph of |π (π₯)| in Figure 1.106. We see that |π (π₯)| is discontinuous only at π₯ = 3, where the graph of |π (π₯)| has a jump.
92
Chapter One /SOLUTIONS |π (π₯)|
3 2 1 1
2
3
4
5
6
π₯
Figure 1.106 64. (a) The initial value is when π‘ = 0, and we see that π (0) = ππβ 0 = π0 = 1000. (b) Since the function is continuous, at π‘ = 12, we have πππ‘ = 100 and we solve for π: π12π = 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 ο¬rst increases linearly for half a second, at the end of which time there is 0.6 ml in the body. Thus, for 0 β€ π‘ β€ 0.5, the function is linear with slope 0.6β0.5 = 1.2: π = 1.2π‘
for
0 β€ π‘ β€ 0.5.
At π‘ = 0.5, we have π = 0.6. For π‘ > 0.5, the quantity decays exponentially at a continuous rate of 0.002, so π has the form 0.5 < π‘. π = π΄πβ0.002π‘ We choose π΄ so that π = 0.6 when π‘ = 0.5: 0.6 = π΄πβ0.002(0.5) = π΄πβ0.001 π΄ = 0.6π0.001 . {
Thus π=
1.2π‘
0 β€ π‘ β€ 0.5
0.6π0.001 πβ.002π‘ 0.5 < π‘. 66. At π₯ = β1, the function is not deο¬ned. Thus, π (π₯) is not continuous at π₯ = β1. We have (π₯ β 1)(π₯ + 1) π₯2 β 1 = lim = lim (π₯ β 1) = β2. π₯ββ1 π₯ββ1 π₯+1 π₯+1 So if we let π (β1) = β2, the function is continuous everywhere. lim
π₯ββ1
67. At π₯ = 5, the function is not deο¬ned. Thus, π(π₯) is not continuous at π₯ = 5. We have (π₯ β 5)(π₯ + 1) π₯2 β 4π₯ β 5 = lim = lim(π₯ + 1) = 6. π₯β5 π₯β5 π₯β5 π₯β5 π₯β5 So if we let π(5) = 6, the function is continuous everywhere. lim
68. At π§ = 9, the function is not deο¬ned. Thus, π (π§) is not continuous at π§ = 9. We have lim π§β9
(π§ β 2)(π§ β 9) 7 π§2 β 11π§ + 18 π§β2 = lim = lim = . π§β9 π§β9 2π§ β 18 2(π§ β 9) 2 2
So if we let π (9) = 7β2, the function is continuous everywhere. 69. At π‘ = 3 and π‘ = β3, the function is not deο¬ned. Thus, π(π‘) is not continuous at π‘ = Β±3. We have lim π‘β3
βπ‘(π‘ β 3)(π‘ + 3) βπ‘3 + 9π‘ = lim = lim βπ‘ = β3. 2 π‘β3 π‘β3 (π‘ β 3)(π‘ + 3) π‘ β9
Similarly, we have
βπ‘(π‘ β 3)(π‘ + 3) βπ‘3 + 9π‘ = lim = lim βπ‘ = 3. 2 π‘ββ3 π‘ββ3 (π‘ β 3)(π‘ + 3) π‘ β9 So if we let π(3) = β3 and π(β3) = 3, the function is continuous everywhere. lim
π‘ββ3
70. At π₯ = 0, the function is not deο¬ned. In addition, limπ₯β0 π (π₯) does not exist. Thus, π (π₯) is not continuous at π₯ = 0.
1.7 SOLUTIONS
93
71. Since limπ₯β0+ π (π₯) = 1 and limπ₯β0β π (π₯) = β1, we see that limπ₯β0 π (π₯) does not exist. Thus, π (π₯) is not continuous at π₯=0 72. Since π₯βπ₯ = 1 for π₯ β 0, this function π (π₯) = 1 for all π₯. Thus, π (π₯) is continuous for all π₯. 73. Since 2π₯βπ₯ = 2 for π₯ β 0, we have limπ₯β0 π (π₯) = 2, so lim π (π₯) β π (0) = 3. π₯β0
Thus, π (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 π(5) < 0 and π(10) > 0 and π(12) < 0, there are two zeros, one between π₯ = 5 and π₯ = 10, and another between π₯ = 10 and π₯ = 12. Thus, π(π₯) is a cubic with at least two zeros. If π(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, π(π₯) cannot have a double zero and have the signs it does. Thus, π(π₯) has three zeros. The third zero can be greater than 12 or less than 5. See Figures 1.107 and 1.108. π(π₯) π₯
π₯ π(π₯)
Figure 1.107
Figure 1.108
76. (a) The graphs of π¦ = ππ₯ and π¦ = 4 β π₯2 cross twice in Figure 1.109. This tells us that the equation ππ₯ = 4 β π₯2 has two solutions. Since π¦ = ππ₯ increases for all π₯ and π¦ = 4 β π₯2 increases for π₯ < 0 and decreases for π₯ > 0, these are only the two crossing points. π¦
π¦ = ππ₯ β2
2
π¦ = π₯2 β 4 π₯
Figure 1.109 (b) Values of π (π₯) are in Table 1.16. One solution is between π₯ = β2 and π₯ = β1; the second solution is between π₯ = 1 and π₯ = 2. Table 1.16 π₯
β4
β3
β2
β1
0
1
2
3
4
π (π₯)
12.0
5.0
0.1
β2.6
β3
β0.3
7.4
25.1
66.6
77. (a) Since π (π₯) is not continuous at π₯ = 1, it does not satisfy the conditions of the Intermediate Value Theorem. (b) We see that π (0) = π0 = 1 and π (2) = 4 + (2 β 1)2 = 5. Since ππ₯ is increasing between π₯ = 0 and π₯ = 1, and since 4 + (π₯ β 1)2 is increasing between π₯ = 1 and π₯ = 2, any value of π between π1 = π and 4 + (1 β 1)2 = 4, such as π = 3, is a value such that π (π₯) = π has no solution.
94
Chapter One /SOLUTIONS
78. A function π¦ = π(π₯) is invertible only if each π¦-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 ο¬nd a value π¦ corresponding to two diο¬erent π₯-values. Since π(π₯) is continuous with π(0) = 3 and π(1) = 8, the Intermediate Value Theorem guarantees that between π₯ = 0 and π₯ = 1, the function π(π₯) takes every value between 3 and 8. We pick any one of the π¦-values between 3 and 8 that is also between 8 and 4. We will pick π¦ = 6, but it could equally well be 5.5 or 7. By the Intermediate Value Theorem, there exists a number π between π₯ = 0 and π₯ = 1 with π(π) = 6. Likewise, since π(π₯) is continuous with π(1) = 8 and π(2) = 4, the Intermediate Value Theorem guarantees that between π₯ = 1 and π₯ = 2, the function π(π₯) takes every value between 4 and 8. In particular, there is a number π between π₯ = 1 and π₯ = 2 with π(π) = 6. This means there are two π₯-values, π₯ = π and π₯ = π, with π between 0 and 1 and π between 1 and 2, so π β π and π(π) = π(π). Thus π(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 π β 2.71828. π¦ 3.5 3 2.5 2 1.5 1 0.5
π¦ = (1 + π₯)1βπ₯
β0.1
0.1
π₯
Figure 1.110
80. We use values of β approaching, but not equal to, zero. If we let β = 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 = β0.01 β0.001, β0.0001, β0.00001, we get values 2.7320, 2.7196, 2.7184, and 2.7183. These numbers suggest that the limit is the number π = 2.71828 β¦. However, these calculations cannot tell us that the limit is exactly π; for that a proof is needed. 81. (a) Since sin(ππ) = 0 for π = 1, 2, 3, β¦ the sequence of π₯-values 1 1 1 , , ,β¦ π 2π 3π works. These π₯-values β 0 and are zeroes of π (π₯). (b) Since sin(ππβ2) = 1 for π = 1, 5, 9 β¦ the sequence of π₯-values 2 2 2 , , ,β¦ π 5π 9π works. (c) Since sin(ππ)β2 = β1 for π = 3, 7, 11, β¦ the sequence of π₯-values 2 2 2 , , β¦ 3π 7π 11π 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 (diο¬erent) values: 0 and 1, or 0 and β1, or 1 and β1. 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 π (π₯) = 5, but it does not tell us which value(s) of π₯ give π (π₯) = 5. 84. For π to be continuous at π₯ = π, we need limπ₯βπ π (π₯) to exist and to be equal to π (π).
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 π (π₯) = β1 π₯ < 15 86. One example is π (π₯) = 1βπ₯, 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₯β€2 87. Let π (π₯) = . Then π (π₯) is continuous at every point in [0, 3] except at π₯ = 2. Other answers are possible. π₯ π₯>2 { π₯ π₯β€3 88. Let π (π₯) = . Then π (π₯) is increasing for all π₯ but π (π₯) is not continuous at π₯ = 3. Other answers are 2π₯ π₯ > 3 possible. { 1 π₯β€3 89. False. For example, let π (π₯) = , then π (π₯) is deο¬ned 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 π (5) < 0. π (π₯)
100
5
10
π₯
Figure 1.111 91. False. A counterexample is graphed in Figure 1.112. π (π)
π (π₯)
π (π)
π
π
π₯
Figure 1.112
Solutions for Section 1.8 EXERCISES 1. (a) As π₯ approaches β1 from the right, π (π₯) approaches 1. So lim+ π (π₯) = 1. π₯ββ1
(b) As π₯ approaches 0 from the left, π (π₯) approaches 0. So limβ π (π₯) = 0. π₯β0
(c) As π₯ approaches 0 from either side, π (π₯) approaches 0, regardless of the fact that π (0) = 2. So lim π (π₯) = 0. π₯β0
(d) As π₯ approaches 1 from the left, π (π₯) approaches 1. So limβ π (π₯) = 1. π₯β1
(e) As π₯ approaches 1 from the left, π (π₯) approaches 1. However, as π₯ approaches 1 from the right, π (π₯) approaches 2. Since there is no single value that π (π₯) approaches as π₯ approaches 1 from both sides, lim π (π₯) does not exist. (f) As π₯ approaches 2 from the left, π (π₯) approaches 1. So limβ π (π₯) = 1. π₯β2
π₯β1
96
Chapter One /SOLUTIONS 2. (a) As π₯ approaches 1 from the left, the values of π (π₯) get closer and closer to 1. So limβ π (π₯) = 1. π₯β1
(b) As π₯ approaches 1 from the right, π (π₯) goes to ββ. So limit does not exist since it does not approach a real number πΏ, but we can use limit notation to say lim+ π (π₯) = ββ. π₯β1
(c) As π₯ approaches 1 from the left, the values of π (π₯) get closer and closer to 1. However, as π₯ approaches 1 from the right, π (π₯) goes to ββ. Since there is no single value that π (π₯) approaches as π₯ approaches 1 from both sides, lim π (π₯) π₯β1
does not exist. (d) As π₯ approaches 2 from the left, the values of π (π₯) get closer and closer to 1. So limβ π (π₯) = 1. π₯β2
(e) As π₯ approaches 2 from the right, the values of π (π₯) get closer and closer to 1. So lim+ π (π₯) = 1. π₯β2
(f) As π₯ approaches 2 from either side, π (π₯) approaches 1, regardless of the fact that π (2) is undeο¬ned. So lim π (π₯) = 1. π₯β2
3. (a) When π₯ = β2, we see that π¦ = 4. Therefore, π (β2) = 4. (b) When π₯ = 0, we see that π¦ = 2. Therefore, π (0) = 2. (c) As π₯ approaches β4 from the right, π (π₯) approaches β4. Therefore, lim+ π (π₯) = β4. π₯ββ4
(d) As π₯ approaches β2 from the left, π (π₯) approaches 2. Therefore, limβ π (π₯) = 2. π₯ββ2
(e) As π₯ approaches β2 from the right, π (π₯) approaches 4. Therefore, lim+ π (π₯) = 4. π₯ββ2
(f) As π₯ approaches 0 from both sides, π (π₯) approaches 0. Therefore, lim π (π₯) = 0. π₯β0
(g) As π₯ approaches 2 from the left, π (π₯) approaches 2. However, as π₯ approaches 2 from the right, π (π₯) approaches 4. Therefore, lim π (π₯) does not exist. π₯β2
(h) As π₯ approaches 4 from the left, π (π₯) approaches 2. Therefore, limβ π (π₯) = 2. π₯β4
4. (a) When π₯ = 0, there is no corresponding value of π¦ on the graph of π . Therefore, π (0) is undeο¬ned. (b) When π₯ = 4, we see that π¦ = β2. Therefore, π (4) = β2. (c) As π₯ approaches β2 from the left, π (π₯) approaches 2. Therefore, limβ π (π₯) = 2. π₯ββ2
(d) As π₯ approaches β2 from the right, π (π₯) approaches β2. Therefore, lim+ π (π₯) = β2. π₯ββ2
(e) From parts (c) and (d), we see that limβ π (π₯) is not equal to lim+ π (π₯). Therefore, lim π (π₯) does not exist. π₯ββ2
π₯ββ2
π₯ββ2
(f) As π₯ approaches 0 from both sides, π (π₯) approaches 2. Therefore, lim π (π₯) = 2. π₯β0
(g) As π₯ approaches 2 from the left, π (π₯) approaches ββ. Therefore, limβ π (π₯) = ββ. π₯β2
(h) As π₯ approaches 2 from the right, π (π₯) approaches β. Therefore, lim+ π (π₯) = β. π₯β2
(i) From parts (g) and (h), we see that limβ π (π₯) is not equal to lim+ π (π₯). Therefore, lim π (π₯) does not exist. π₯β2
π₯β2
π₯β2
(j) As π₯ approaches 4 from the left, π (π₯) approaches 2. However, as π₯ approaches 4 from the right, π (π₯) approaches β2. Therefore, lim π (π₯) does not exist. π₯β4
5. (a) As π₯ gets larger and larger, the values of π (π₯) oscillate, but the oscillations get smaller and smaller around 3. Therefore, we estimate that lim π (π₯) = 3 π₯ββ
(b) As π₯ gets larger and larger in magnitude but negative, the values of π (π₯) get larger and larger in magnitude but negative, so the π (π₯) does not approach a real number, so the limit does not exist. Alternatively, we can say lim π (π₯) = ββ. π₯βββ
6. Using Theorem 1.2 we have, lim(π (π₯) β 2β(π₯)) = lim π (π₯) β lim 2β(π₯)
Property 2
= lim π (π₯) β 2 lim β(π₯) π₯β2 π₯β2 1 = 7 β 2 β = 6. 2
Property 1
π₯β2
π₯β2
π₯β2
7. Using Theorem 1.2 we have, lim(π(π₯))2 = lim(π(π₯) β π(π₯)) π₯β2
π₯β2
= (lim π(π₯)) β (lim π(π₯)) Property 3 π₯β2
π₯β2
= (β4)(β4) = 16. 8. Using Theorem 1.2 we have, lim
π (π₯)
π₯β2 π(π₯) β β(π₯)
=
limπ₯β2 π (π₯) limπ₯β2 (π(π₯) β β(π₯))
Property 4
1.8 SOLUTIONS limπ₯β2 π (π₯) (limπ₯β2 π(π₯))(limπ₯β2 β(π₯)) 7 7 =β . = 1 2 (β4)( 2 ) =
9. We have
97
Property 3
lim(π (π₯) + π(π₯)) = lim π (π₯) + lim π(π₯) = 27 + 3 = 30. π₯βπ
10. We have
π₯βπ
π₯βπ
lim(π (π₯) β π(π₯)) = lim π (π₯) β lim π(π₯) = 27 β 3 = 24. π₯βπ
11. We have
π₯βπ
π₯βπ
lim(π (π₯)π(π₯)) = lim(π (π₯)) β lim(π(π₯)) = 27 β 3 = 81. π₯βπ
π₯βπ
12. Since limπ₯βπ π(π₯) β 0, we have
( lim π₯βπ
13. We have
π (π₯) π(π₯)
π₯βπ
) =
limπ₯βπ π (π₯) 27 = = 9. limπ₯βπ π(π₯) 3
( ) lim 10(π (π₯) β π(π₯)) = 10 lim π (π₯) β lim π(π₯) = 10 (27 β 3) = 240. π₯βπ
14. We have
π₯βπ
π₯βπ
( )( ) lim(π(π₯))2 = lim(π(π₯) β π(π₯)) = lim π(π₯) lim π(π₯) = 32 = 9. π₯βπ
π₯βπ
π₯βπ
π₯βπ
15. From the graphs of π and π, we estimate limβ π (π₯) = 3, limβ π(π₯) = 5, π₯β1
lim+ π (π₯) = 4, lim+ π(π₯) = 1.
π₯β1
π₯β1
π₯β1
(a) Using Theorem 1.2 we have limβ (π (π₯) + π(π₯)) = 3 + 5 = 8. π₯β1
(b) Using Theorem 1.2 we have lim+ (π (π₯) + 2π(π₯)) = lim+ π (π₯) + 2 lim+ π(π₯) = 4 + 2(1) = 6 π₯β1
π₯β1
π₯β1
(c) Using Theorem 1.2 we have limβ (π (π₯)π(π₯)) = ( limβ π (π₯))( limβ π(π₯)) = (3)(5) = 15 π₯β1 π₯β1 π₯β1 ( ) ( ) (d) Using Theorem 1.2 we have lim+ (π (π₯)βπ(π₯)) = lim+ π (π₯) β lim+ π(π₯) = 4β1 = 4 π₯β1
π₯β1
π₯β1
16. We see that π (π₯) goes to ββ 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 π (π₯) goes to β on the left and to ββ 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 π (π₯) goes to β on the left and approaches a π¦-value of 1 on the right. One possible graph is shown in Figure 1.115. Other answers are possible. π¦
1
π₯
Figure 1.115
19. We see that π (π₯) approaches a π¦-value of 3 on the left and goes to ββ on the right. One possible graph is shown in Figure 1.116. Other answers are possible. π¦ 3 π₯
Figure 1.116
20. We see that π (π₯) goes to β on the right and that it also passes through the point (β1, 2). (Notice that this must be a point on the graph since the instructions require that π (π₯) be deο¬ned and continuous.) One possible graph is shown in Figure 1.117. Other answers are possible.
2 π₯
β1
Figure 1.117
21. We see that π (π₯) goes to β 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 π (π₯) be deο¬ned 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 = β because π₯2 increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large and π₯ββ positive. 23. We have lim π₯2 = β because π₯2 increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large in π₯βββ magnitude and negative. 24. We have lim π₯3 = ββ because π₯3 decreases and becomes arbitrarily large in magnitude and negative as π₯ becomes π₯βββ arbitrarily large in magnitude and negative. 25. We have lim π₯3 = β because π₯3 increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large and π₯ββ positive. 26. We have lim ππ₯ = β because ππ₯ increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large and π₯ββ positive. 1 27. We have lim πβπ₯ = lim π₯ = 0 because ππ₯ increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily π₯ββ π₯ββ π large and positive, so 1βππ₯ gets closer and closer to 0 as π₯ becomes arbitrarily large and positive. 1 28. We have lim 5βπ₯ = lim π₯ = 0 because 5π₯ increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily π₯ββ π₯ββ 5 large and positive, so 1β5π₯ gets closer and closer to 0 as π₯ becomes arbitrarily large and positive. β β 29. We have lim π₯ = β because π₯ increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large and π₯ββ positive. 30. We have lim ln π₯ = β because ln π₯ increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily large and π₯ββ positive. 1 31. We have lim π₯β2 = lim 2 = 0 because π₯2 increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily π₯ββ π₯ββ π₯ large and positive, so 1βπ₯2 gets closer and closer to 0 as π₯ becomes arbitrarily large and positive. 1 32. We have lim π₯β2 = lim 2 = 0 because π₯2 increases and becomes arbitrarily large and positive as π₯ becomes arbitrarily π₯βββ π₯βββ π₯ large in magnitude and negative, so 1βπ₯2 gets closer and closer to 0 as π₯ becomes arbitrarily large in magnitude and negative. 1 33. We have lim π₯β3 = lim 3 = 0 because π₯3 decreases and becomes arbitrarily large in magnitude and negative as π₯ π₯βββ π₯βββ π₯ becomes arbitrarily large in magnitude and negative, so 1βπ₯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₯ββ 2 π₯ββ 2 large and positive, so 1β2π₯ gets closer and closer to 0 as π₯ becomes arbitrarily large and positive. 35. We see that lim π (π₯) = ββ and lim π (π₯) = ββ. π₯βββ
π₯ββ
36. As π₯ β Β±β, we know that π (π₯) behaves like its leading term β2π₯3 . Thus, we have lim π (π₯) = β and lim π (π₯) = ββ. π₯βββ
π₯ββ
37. As π₯ β Β±β, we know that π (π₯) behaves like its leading term π₯5 . Thus, we have lim π (π₯) = ββ and lim π (π₯) = β. π₯βββ
π₯ββ
38. As π₯ β Β±β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π (π₯) β
3 3π₯3 = , 5 5π₯3
we have lim π (π₯) = 3β5 and lim π (π₯) = 3β5. π₯βββ
π₯ββ
39. As π₯ β Β±β, we know that π₯β3 gets closer and closer to zero, so we have lim π (π₯) = 0 and lim π (π₯) = 0. π₯βββ
π₯ββ
40. We have lim π (π₯) = 0 and lim π (π₯) = β. π₯βββ
π₯ββ
|π₯| |π₯| |π₯| = 1 and limβ = β1, we say that lim does not exist. In addition π (π₯) is not deο¬ned at 0. Therefore, 41. Since lim+ π₯β0 π₯β0 π₯ π₯β0 π₯ π₯ π (π₯) is not continuous on any interval containing 0. { β§ π₯β4 π₯>4 |π₯ β 4| βͺ π₯ β 4 1 π₯>4 =β¨ π₯β4 = 42. π (π₯) = π₯β4 β1 π₯ < 4 π₯<4 βͺβ β© π₯β4 Figure 1.119 conο¬rms that lim+ π (π₯) = 1, limβ π (π₯) = β1 so lim π (π₯) does not exist. π₯β4
π₯β4
π₯β4
100
Chapter One /SOLUTIONS π (π₯)
1
0
2
4
6
π₯
8
β1
Figure 1.119 β§ π₯β2 , π₯>2 βͺ π₯ |π₯ β 2| βͺ 43. π (π₯) = =β¨ π₯ βͺ π₯β2 βͺβ π₯ , π₯ < 2 β© Figure 1.120 conο¬rms that lim+ π (π₯) = limβ π (π₯) = lim π (π₯) = 0. π₯β2
π₯β2
π₯β2
1
π (π₯)
0
1
2
3
4
π₯
Figure 1.120 β§ π₯2 β 2 0 < π₯ < 3 βͺ 44. π (π₯) = β¨ 2 π₯=3 βͺ 3<π₯ β© 2π₯ + 1 Figure 1.121 conο¬rms that limβ π (π₯) = limβ (π₯2 β 2) = 7 and that lim π (π₯) = lim (2π₯ + 1) = 7, so lim π (π₯) = 7. π₯β3
π₯β3
π₯β3+
Note, however, that π (π₯) is not continuous at π₯ = 3 since π (3) = 2. π¦ 10 8 6 4 2 0 β2
π (π₯)
1
2
3
4
5
π₯
Figure 1.121 45. Yes. Since lim π (π₯) = limβ (π₯2 + 1) = 2
π₯β1β
π₯β1
lim+ π (π₯) = lim+ 2π₯ = 2,
π₯β1
π₯β1
we deο¬ne π (1) = 2. 46. No. Since lim π (π₯) = limβ (4 β π₯2 ) = 3
π₯β1β
π₯β1
lim+ π (π₯) = lim+ (π₯ + 1) = 2.
π₯β1
π₯β1
π₯β3+
π₯β3
1.8 SOLUTIONS
101
47. Yes. Since lim π (π₯) = limβ (π₯ β 1) = 0
π₯β1β
π₯β1
lim+ π (π₯) = lim+ (2 β 2π₯) = 0,
π₯β1
π₯β1
we deο¬ne π (1) = 0. 48. No. Since 1 = Not deο¬ned (or +β) 1βπ₯ lim+ π (π₯) = lim+ π₯ = 1.
lim π (π₯) = limβ
π₯β1β
π₯β1
π₯β1
π₯β1
PROBLEMS 49. The graph in Figure 1.122 suggests that as π₯ grows large, the value of (1 + 1βπ₯)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 π β 2.71828. Thus we guess that lim (1 + 1βπ₯)π₯ = π π₯ββ
π¦ 5
π¦=π
π (π₯) = (1 + 1βπ₯)π₯
β10
10
100
π₯
Figure 1.122 50. We use values of π₯ approaching β and make a table. We see that as π₯ grows very large, the value of (1 + 1βπ₯)π₯ appears to approach a value close to 2.7183. We recognize this value as π rounded to four decimal places, so we estimate lim (1 + π₯ββ
1βπ₯)π₯ = π. π₯
1
10
100
1000
10000
100000
1000000
(1 + 1βπ₯)π₯
2.0000
2.5937
2.7048
2.7169
2.7181
2.7183
2.7183
51. (a)
10
5
β10
β5
5
10
π₯
Figure 1.123 (b) The graph of π (π₯) suggests that it is not continuous at π₯ = 0. However, the function π (π₯) is the composition of a rational function 1β(π₯2 + 0.0001), which is continuous everywhere since its denominator is never zero, with the exponential function ππ₯ , which is continuous everywhere. Therefore π (π₯) is continuous everywhere, so must be continuous at π₯ = 0.
Chapter One /SOLUTIONS
102
52. When π₯ = 0.1, we ο¬nd π₯π1βπ₯ β 2203. When π₯ = 0.01, we ο¬nd π₯π1βπ₯ β 3 Γ 1041 . When π₯ = 0.001, the value of π₯π1βπ₯ is too big for a calculator to compute. This suggests that lim+ π₯π1βπ₯ does not exist (and in fact it does not). π₯β0
53. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π₯ π (π₯) β = β1, βπ₯ we have lim π (π₯) = β1. π₯ββ Alternatively, we could divide numerator and denominator by π₯ and apply the properties of limits: π (π₯) = so
1 + 3βπ₯ π₯+3 = , 2βπ₯ 2βπ₯ β 1
lim (1 + 3βπ₯) lim 1 + lim (3βπ₯) 1 + 3βπ₯ π₯ββ π₯ββ π₯ββ 1 = = = β1 = π₯ββ 2βπ₯ β 1 lim (2βπ₯ β 1) lim (2βπ₯) β lim 1 β1
lim π (π₯) = lim
π₯ββ
π₯ββ
π₯ββ
π₯ββ
since 1βπ₯ β 0 as π₯ β β. 54. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π (π₯) β
3 3π₯ = , ππ₯ π
we have lim π (π₯) = 3βπ. π₯ββ Alternatively, we could divide numerator and denominator by π₯ and apply the properties of limits: πβπ₯ + 3 π + 3π₯ = , ππ₯ β 3 π β 3βπ₯
π (π₯) = so
lim (πβπ₯ + 3) lim (πβπ₯) + lim 3 πβπ₯ + 3 π₯ββ π₯ββ π₯ββ 3 = = = π₯ββ π β 3βπ₯ lim (π β 3βπ₯) lim π β lim (3βπ₯) π
lim π (π₯) = lim
π₯ββ
π₯ββ
π₯ββ
π₯ββ
since πβπ₯ β 0 as π₯ β β for any nonzero number π.. 55. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π (π₯) β
1 π₯ = , 2π₯ 2π₯2
we have lim π (π₯) = 0 because 1β(2π₯) β 0 as π₯ β β. π₯ββ
Alternatively, we could divide numerator and denominator by π₯2 and apply the properties of limits: π (π₯) =
1βπ₯ β 5βπ₯2 π₯β5 , = 5 + 2π₯2 5βπ₯2 + 2
) ( lim (1βπ₯) β lim (5βπ₯2 ) lim (1βπ₯) β (5βπ₯2 ) 1βπ₯ β 5βπ₯2 π₯ββ π₯ββ π₯ββ 0 = =0 lim π (π₯) = lim = ) = ( π₯ββ π₯ββ 5βπ₯2 + 2 2 lim (5βπ₯2 ) + lim 2 lim (5βπ₯2 ) + 2
so
π₯ββ
since lim πβπ₯π = 0 for any nonzero number π and positive π.
π₯ββ
π₯ββ
π₯ββ
56. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π (π₯) β
1 π₯2 = , 3 3π₯2
we have lim π (π₯) = 1β3. π₯ββ
Alternatively, we could divide numerator and denominator by π₯2 and apply the properties of limits: π (π₯) =
1 + 2βπ₯ β 1βπ₯2 π₯2 + 2π₯ β 1 , = 2 3 + 3π₯ 3βπ₯2 + 3
( ) lim 1 + lim (2βπ₯) β lim (1βπ₯2 ) lim 1 + 2βπ₯ β 1βπ₯2 1 + 2βπ₯ β 1βπ₯2 π₯ββ π₯ββ π₯ββ π₯ββ 1 lim π (π₯) = lim = = = ) ( π₯ββ π₯ββ 3 3βπ₯2 + 3 lim (3βπ₯2 ) + lim 3 lim 3βπ₯2 + 3
so
π₯ββ
since lim πβπ₯π = 0 for any nonzero number π and positive π. π₯ββ
π₯ββ
π₯ββ
1.8 SOLUTIONS
103
57. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π₯2 = π₯, π₯
π (π₯) β
we have lim π (π₯) = β. π₯ββ Alternatively, we could divide numerator and denominator by π₯ and apply the properties of limits: π₯ + 4βπ₯ π₯2 + 4 = , π₯+3 1 + 3βπ₯
π (π₯) = so
lim (π₯ + 4βπ₯) lim π₯ + lim (4βπ₯) π₯ + 4βπ₯ π₯ββ π₯ββ π₯ββ = = lim π₯ = β = π₯ββ 1 + 3βπ₯ lim (1 + 3βπ₯) lim 1 + lim (3βπ₯) π₯ββ
lim π (π₯) = lim
π₯ββ
π₯ββ
π₯ββ
π₯ββ
since lim πβπ₯ = 0 for any nonzero number π. π₯ββ
58. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π (π₯) β
2π₯3 2 = , 3 3π₯3
we have lim π (π₯) = 2β3. π₯ββ
Alternatively, we could divide numerator and denominator by π₯3 and apply the properties of limits: π (π₯) = so
2 β 16βπ₯ 2π₯3 β 16π₯2 = , 2 3 4βπ₯ + 3 4π₯ + 3π₯
lim (2 β 16βπ₯) lim 2 β lim (16βπ₯) 2 β 16βπ₯ π₯ββ π₯ββ π₯ββ 2 = = = π₯ββ 4βπ₯ + 3 lim (4βπ₯ + 3) lim (4βπ₯) + lim 3 3
lim π (π₯) = lim
π₯ββ
π₯ββ
π₯ββ
π₯ββ
since lim πβπ₯ = 0 for any nonzero number π. π₯ββ
59. As π₯ β β, we know that π (π₯) behaves like the quotient of the leading terms of its numerator and denominator. Since π₯4 1 = , 2π₯ 2π₯5
π (π₯) β we have lim π (π₯) = 0 because 1β(2π₯) β 0 as π₯ β β. π₯ββ
Alternatively, we could divide numerator and denominator by π₯5 and apply the properties of limits: π (π₯) =
1βπ₯ + 3βπ₯4 π₯4 + 3π₯ = , 4 5 1βπ₯ + 2 π₯ + 2π₯
( ) lim 1βπ₯ + 3βπ₯4
so lim π (π₯) =
π₯ββ
π₯ββ
lim (1βπ₯ + 2)
lim (1βπ₯) + lim (3βπ₯4 )
=
π₯ββ
π₯ββ
=
lim (1βπ₯) + lim 2
π₯ββ
π₯ββ
π₯ββ
0 =0 2
since lim πβπ₯π = 0 for any nonzero number π and positive π. π₯ββ
60. For large values of π₯, 3ππ₯ + 2 behaves like 3ππ₯ and 2ππ₯ + 3 behaves like 2ππ₯ , so for large values of π₯, π (π₯) β
3 3ππ₯ = . 2ππ₯ 2
Thus we have we have lim π (π₯) = 3β2. π₯ββ Alternatively, we could divide numerator and denominator by ππ₯ and apply the properties of limits: π (π₯) = so
3 + 2πβπ₯ 3ππ₯ + 2 , = 2ππ₯ + 3 2 + 3πβπ₯
lim (3 + 2πβπ₯ )
lim π (π₯) =
π₯ββ
π₯ββ π₯ββ
since lim ππβπ₯ = 0 for any nonzero number π. π₯ββ
lim (2 + 3πβπ₯ )
lim 3 + lim 2πβπ₯
=
π₯ββ
π₯ββ
lim 2 + lim 3πβπ₯
π₯ββ
π₯ββ
=
3 2
104
Chapter One /SOLUTIONS
61. Since lim 2βπ₯ = lim 3βπ₯ = 0, we have π₯ββ
π₯ββ
lim (2βπ₯ + 5) lim 2βπ₯ + lim 5 π₯ββ π₯ββ π₯ββ 5 2βπ₯ + 5 lim π (π₯) = lim βπ₯ = = = . π₯ββ π₯ββ 3 +7 lim (3βπ₯ + 7) lim 3βπ₯ + lim 7 7 π₯ββ
π₯ββ
π₯ββ
62. Since lim ππβπ₯ = 0 for any nonzero π, we have π₯ββ
lim (2πβπ₯ + 3)
lim π (π₯) =
π₯ββ
π₯ββ
lim (3πβπ₯ + 2)
lim 2πβπ₯ + lim 3
=
π₯ββ
π₯ββ
π₯ββ
lim 3πβπ₯ + lim 2
π₯ββ
π₯ββ
=
3 . 2
63. (a) Figure 1.124 shows a possible graph of π (π₯), yours may be diο¬erent. 9
2 3
π₯
5
Figure 1.124 (b) In order for π to approach the horizontal asymptote at 9 from above it is necessary that π eventually become concave up. It is therefore not possible for π to be concave down for all π₯ > 6. 64. One possible graph is shown in Figure 1.125. Other answers are possible. π¦ 4
β4
π₯
4 β2
Figure 1.125 65. One possible graph is shown in Figure 1.126. Other answers are possible. π¦ 4
β5
5 β3
Figure 1.126
π₯
1.8 SOLUTIONS
105
66. (a) We know that lim π (π₯) does not exist for π = 3. Since the graph of π (π₯) has a vertical asymptote at π₯ = 3, this π₯βπ
means that π (π₯) approaches β or ββ as π₯ approaches 3 from the right or from the left. This means that π (π₯) cannot approach a ο¬nite real number as π₯ approaches 3 from both sides. (b) If lim π (π₯) exists, then the graph of π (π₯) must approach a horizontal asymptote as π₯ approaches β. Since the only π₯ββ
horizontal asymptote is π¦ = β4, the value of π (π₯) must approach β4 as π₯ gets large. So lim π (π₯) = β4. π₯ββ
67. (a)
(i) As π‘ approaches 1 from the left, π approaches 50. Therefore, limβ π (π‘) = 50. This means that the amount of the π‘β1
drug in the patientβs body is about 50 mg right before the second dose is taken. (ii) As π‘ approaches 1 from the right, π approaches 150. Therefore, lim+ π (π‘) = 150. This means that the amount of π‘β1
drug in the patientβs body is about 150 mg right after the second dose is taken. (b) The function π is discontinuous at π‘ = 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₯ suο¬ciently close to π₯ = 1 but with π₯ > 1, we have π(π₯) = 14, so lim+ π(π₯) = 14. For all π₯ suο¬ciently close to π₯β1
π₯ = 1 but with π₯ < 1 we have π(π₯) = 7, so limβ π(π₯) = 7. Therefore, the one sided limits of π(π₯) at π₯ = 1 are diο¬erent and π₯β1
so lim π(π₯) does not exist. π₯β1
69. We calculate this limit in stages, using the limit properties in Theorem 1.2 to justify each step: ) ( lim π₯2 + 5π₯ π₯β3 π₯2 + 5π₯ (Property 4, since limπ₯β3 (π₯ + 9) β 0) lim = π₯β3 π₯ + 9 lim (π₯ + 9) π₯β3 ( ) lim π₯2 + lim (5π₯) π₯β3 π₯β3 = (Property 2) lim π₯ + lim 9 π₯β3 π₯β3 ( )2 ( ) lim π₯ + 5 lim π₯ π₯β3 π₯β3 = (Properties 1 and 3) lim π₯ + lim 9 π₯β3
π₯β3
32 + 5 β 3 = = 2. 3+9
(Properties 5 and 6)
70. There are many possible correct answers. (a) If π (π₯) = π₯2 and π(π₯) = π₯ then π (π₯)βπ(π₯) = π₯ so lim
π (π₯)
π₯ββ π(π₯)
(b) If π (π₯) = 3π₯ and π(π₯) = π₯ then π (π₯)βπ(π₯) = 3 so lim
π (π₯)
π₯ββ π(π₯)
(c) If π (π₯) = π₯ and π(π₯) = π₯2 then π (π₯)βπ(π₯) = 1βπ₯ so lim
= β. = 3.
π (π₯)
π₯ββ π(π₯)
= 0.
71. (a) We have π₯+5 10 10 1 = β β π₯ β 5 π₯2 β 5 (π₯ + 5)(π₯ β 5) (π₯ + 5)(π₯ β 5) π₯ + 5 β 10 = (π₯ + 5)(π₯ β 5) π₯β5 . = (π₯ + 5)(π₯ β 5) (b) We have lim π₯β5
(
10 1 β π₯ β 5 π₯2 β 25
)
π₯β5
= lim
π₯β5 (π₯ + 5)(π₯ β 5)
= lim
1
π₯β5 π₯ + 5
=
1 1 = 5+5 10
Canceling π₯ β 5 since π₯ β 5 in the limit Substituting π₯ = 5 since 1β(π₯ + 5) is continuous at π₯ = 5.
106
Chapter One /SOLUTIONS (c) Property 2 of Theorem 1.2 states lim(π (π₯) + π(π₯)) = lim π (π₯) + lim π(π₯) π₯βπ
π₯βπ
π₯βπ
provided the limits on the right hand side exist. In this case, neither lim
1
π₯β5 π₯ β 5
invoke the property.
10 exist, so we cannot nor lim β 2 π₯β5 π₯ β 25
72. The only change is that, instead of considering all π₯ near π, we only consider π₯ near to and greater than π. Thus we deο¬ne limπ₯βπ + π (π₯), to be a number πΏ (if one exists) such that π (π₯) is as close to πΏ as we want whenever π₯ is suο¬ciently close to π and π₯ > π. 73. The only change is that, instead of considering all π₯ near π, we only consider π₯ near to and less than π. Thus we deο¬ne limπ₯βπ β π (π₯), to be a number πΏ (if one exists) such that π (π₯) is as close to πΏ as we want whenever π₯ is suο¬ciently close to π and π₯ < π. 74. If π is in the interval, we know lim π (π₯) = π (π) and limπ₯βπ π(π₯) = π(π). Then, π₯βπ
lim (π (π₯) + π(π₯)) = lim π (π₯) + lim π(π₯) Property 2 π₯βπ
π₯βπ
π₯βπ
= π (π) + π(π),
so π + π is continuous at π₯ = π.
Also, lim (π (π₯)π(π₯)) = lim π (π₯) lim π(π₯) Property 3 π₯βπ
π₯βπ
π₯βπ
= π (π)π(π) so π π is continuous at π₯ = π. Finally,
lim
π (π₯)
π₯βπ π(π₯)
limπ₯βπ π (π₯) Property 4 limπ₯βπ π(π₯) π (π) π = , so is continuous at π₯ = π. π(π) π =
Strengthen Your Understanding 75. Though π (π₯) and π(π₯) are both continuous for all π₯, it is possible for π(π₯) to be equal to zero for some π₯. For any such value of π₯, where π(π₯) = 0, we see that π (π₯)βπ(π₯) is undeο¬ned, and thus not continuous. For example, π (π₯) π₯ = π(π₯) π₯β1 is not deο¬ned or continuous at π₯ = 1. 76. The left- and right-hand limits are not the same: lim
π₯β1
= β1,
lim
π₯β1
= 1.
π₯β1β |π₯ β 1|
but
π₯β1+ |π₯ β 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 π (π₯) = We have limπ₯β1 π (π₯) = 4 but π (1) is undeο¬ned.
(π₯ + 3)(π₯ β 1) . π₯β1
78. One example is π (π₯) =
2|π₯| . π₯
1.8 SOLUTIONS
107
79. True, by Property 3 of limits in Theorem 1.2, since lim π₯ = 3. π₯β3
80. False. If lim π(π₯) does not exist, then lim π (π₯)π(π₯) may not even exist. For example, let π (π₯) = 2π₯ + 1 and deο¬ne π by: π₯β3
π₯β3
{
1β(π₯ β 3) if π₯ β 3 4 if π₯ = 3 Then lim π (π₯) = 7 and π(3) = 4, but lim π (π₯)π(π₯) β 28, since lim(2π₯ + 1)β(π₯ β 3) does not exist. π(π₯) =
π₯β3
π₯β3
π₯β3
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 π(π₯) = lim(π (π₯) + π(π₯) + (β1)π (π₯)) = lim (π (π₯) + π(π₯)) + (β1) lim π (π₯) = 12 + (β1)7 = 5. π₯β3
π₯β3
π₯β3
π₯β3
83. True. Suppose instead that lim π(π₯) does not exist but lim(π (π₯)π(π₯)) did exist. Since lim π (π₯) exists and is not zero, then π₯β3
π₯β3
π₯β3
lim((π (π₯)π(π₯))βπ (π₯)) exists, by Property 4 of limits in Theorem 1.2. Furthermore, π (π₯) β 0 for all π₯ in some interval π₯β3
about 3, so (π (π₯)π(π₯))βπ (π₯) = π(π₯) for all π₯ in that interval. Thus lim π(π₯) exists. This contradicts our assumption that π₯β3
lim π(π₯) does not exist. π₯β3
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 β1. 87. False, since we donβt know if π (π₯) or (π (π₯))2 is deο¬ned at π₯ = 7. 88. False, since limπ₯β7 π (π₯) does not exist. 89. True, since limπ₯β7 (π (π₯))2 = 4 and (π (7)2 ) = 4. 90. True, since as π₯ β β, 1βπ₯ β 0 and as the sine function is continuous, sin(1βπ₯) β 0, so the product of the two has a limit of 0. 91. False, since as π₯ β 0+ the function 1βπ₯ β β. Also, as π₯ β β the function sin(1βπ₯) oscillates faster and faster between +1 and β1. Therefore the product of the two does not tend to either β or ββ 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 π (π₯) is the product of the rational function 1β(π₯2 β 1) with πsin(3π₯ +2π₯β1) . 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₯)βπ₯
so, lim
π₯
π₯β0 sin π₯
=
limπ₯β0 1 1 = = 1. limπ₯β0 (sin π₯)βπ₯ 1
94. We have sin π₯ = π₯ Therefore,
sin π₯ . π₯
) ( )( sin π₯ = 0 β 1 = 0. lim sin π₯ = lim π₯ lim π₯β0 π₯β0 π₯β0 π₯
95. We have (sin 3π₯)βπ₯ = 3(sin 3π₯)β(3π₯). If we let π’ = 3π₯, then π’ β 0 as π₯ β 0, so lim π₯β0
Thus lim π₯β0
sin 3π₯ sin π’ = lim = 1. π’β0 3π₯ π’
sin 3π₯ sin 3π₯ = 3 lim = 3. π₯β0 3π₯ π₯
108
Chapter One /SOLUTIONS
96. We have
β sin2 π₯ cos2 π₯ β 1 = . π₯2 π₯2
Therefore
)( ) ( cos2 π₯ β 1 sin π₯ sin π₯ lim = β1 = β lim 2 π₯β0 π₯β0 π₯ π₯ π₯ 97. (a) This statement follows: if we interchange the roles of π and π 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 π(π) = 0. (c) This follows, since if π(π) β 0 the original statement would imply π βπ is continuous at π₯ = π, but we are told it is not. (d) This does not follow. Given that π is continuous at π₯ = π and π(π) β 0, then the original statement says π continuous implies π βπ continuous, not the other way around. In fact, statement (d) is not true: if π (π₯) = 0 for all π₯, then π could be any discontinuous, non-zero function, and π βπ would be zero, and therefore continuous. Thus the conditions of the statement would be satisο¬ed, but not the conclusion. lim π₯β0
Solutions for Section 1.9 EXERCISES 1. Canceling, we have lim
3π₯2 = lim 3 = 3. π₯β0 π₯2
lim
3π₯2 = lim 3π₯ = 0. π₯β0 π₯
lim
3π₯2 3 = lim 2 = β. π₯β0 π₯ π₯4
π₯β0
2. Canceling, we have π₯β0
3. The limit does not exist since canceling, we have π₯β0
4. Factoring the numerator and simplifying, we get π₯(π₯ β 3) π₯2 β 3π₯ = =π₯ π₯β3 π₯β3 provided π₯ β 3. Thus lim π₯β3
π₯2 β 3π₯ = lim π₯ = 3. π₯β3 π₯β3
5. Factoring the numerator and the denominator, we obtain π‘2 (π‘2 + 1) π‘2 + 1 π‘4 + π‘2 = = 2π‘ β 9 2π‘3 β 9π‘2 π‘2 (2π‘ β 9) provided π‘ β 0. Thus lim
π‘4 + π‘2
π‘β0 2π‘3 β 9π‘2
6. Factoring the numerator, we obtain
provided π₯ β 0. Thus
= lim
π‘2 + 1
π‘β0 2π‘ β 9
1 =β . 9
π₯(π₯2 β 3) π₯2 β 3 π₯3 β 3π₯ = β = β β 2π₯ + 3 π₯ 2π₯ + 3 π₯ 2π₯ + 3 β 3 π₯3 β 3π₯ π₯2 β 3 lim β = lim β = β β = β 3. π₯β0 π₯β0 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₯ β 3) 2π₯ β 3 2π₯2 + 5π₯ β 12 provided π₯ β β4. Thus
π₯+4
lim
π₯ββ4 2π₯2 + 5π₯ β 12
= lim
1
π₯ββ4 2π₯ β 3
=β
1 . 11
8. Factoring the numerator and simplifying, we get (π¦ β 1)(π¦ β 4) π¦2 β 5π¦ + 4 = =π¦β4 π¦β1 π¦β1 provided π¦ β 1. Thus
π¦2 β 5π¦ + 4 = lim(π¦ β 4) = β3. π¦β1 π¦β1 π¦β1
lim
9. Factoring the numerator and denominator and simplifying, we get (π₯ β 1)(π₯ + 3) π₯+3 π₯2 + 2π₯ β 3 = = (π₯ β 1)(π₯ β 2) π₯β2 π₯2 β 3π₯ + 2 provided π₯ β 1. Thus
π₯2 + 2π₯ β 3 π₯+3 = lim = β4. π₯β1 π₯2 β 3π₯ + 2 π₯β1 π₯ β 2
lim
10. Factoring the numerator and denominator and simplifying, we get (π‘ + 2)(2π‘ β 1) 2π‘ β 1 2π‘2 + 3π‘ β 2 = = (π‘ + 2)(π‘ + 3) π‘+3 π‘2 + 5π‘ + 6 provided π‘ β β2. Thus
2π‘2 + 3π‘ β 2 2π‘ β 1 = lim = β5. π‘ββ2 π‘2 + 5π‘ + 6 π‘ββ2 π‘ + 3 lim
11. Factoring the numerator and the denominator and simplifying, we get (π₯ β 3)(π₯ + 3) π₯+3 π₯2 β 9 = = (π₯ β 3)(π₯ + 4) π₯+4 π₯2 + π₯ β 12 provided π₯ β 3. Thus lim
π₯2 β 9
π₯β3 π₯2 + π₯ β 12
= lim
π₯+3
π₯β3 π₯ + 4
=
6 . 7
12. Factoring the numerator and the denominator, we obtain (2π¦ β 1)(π¦ + 1) 2π¦ β 1 2π¦2 + π¦ β 1 = = (3π¦ β 1)(π¦ + 1) 3π¦ β 1 3π¦2 + 2π¦ β 1 provided π¦ β β1. Thus
2π¦2 + π¦ β 1 2π¦ β 1 3 = lim = . π¦ββ1 3π¦2 + 2π¦ β 1 π¦ββ1 3π¦ β 1 4 lim
13. Expanding the numerator, we get
(3 + β)2 β 9 = 9 + 6β + β2 β 9 = 6β + β2 .
Next, factoring and simplifying, we get β(6 + β) (3 + β)2 β 9 = =6+β β β provided β β 0. Thus
(3 + β)2 β 9 = lim(6 + β) = 6. ββ0 ββ0 β lim
109
110
Chapter One /SOLUTIONS
14. Simplifying and factoring the numerator and the denominator, we obtain (π₯ + 3)(π₯ + 7) (π₯ + 5)2 β 4 π₯2 + 10π₯ + 21 π₯+7 = = = 2 (π₯ + 3)(π₯ β 3) π₯β3 π₯ β9 π₯2 β 9 provided π₯ β β3. Thus lim
π₯ββ3
(π₯ + 5)2 β 4 2 π₯+7 = lim =β . π₯ββ3 π₯ β 3 3 π₯2 β 9
15. Factoring the numerator and the denominator, we obtain 5(π₯2 β 3) 5 5π₯2 β 15 = 2 = 2 4 π₯ β9 (π₯ β 3)(π₯2 + 3) π₯ +3 provided π₯ β
β
3. Thus
5 5π₯2 β 15 5 = lim = . β 4 2 6 π₯β 3 π₯ β 9 π₯β 3 π₯ + 3 lim β
16. Rewriting the numerator as a single quotient we get 2βπ₯ β 1 = (2 β π₯)βπ₯. Then (2 β π₯)βπ₯ 2βπ₯ β 1 1 = =β π₯β2 π₯β2 π₯ provided π₯ β 2. Thus lim π₯β2
17. Simplifying, we obtain
2βπ₯ β 1 1 1 = lim β = β . π₯β2 π₯ π₯β2 2
3βπ‘
1βπ‘ β 1β3 β(π‘ β 3) 3βπ‘ 1 β1 = 3π‘ = β = = π‘β3 π‘β3 3π‘ π‘β3 3π‘(π‘ β 3) 3π‘ provided π‘ β 3. Thus lim π‘β3
1βπ‘ β 1β3 1 β1 = lim =β . π‘β3 3π‘ π‘β3 9
18. Rewriting the numerator as a single quotient, we have 1 β (π‘ + 1) 1 π‘ β1= =β π‘+1 π‘+1 π‘+1 Then
1β(π‘ + 1) β 1 π‘β(π‘ + 1) 1 =β =β π‘ π‘ π‘+1
provided π‘ β 0. Thus
lim π‘β0
1β(π‘ + 1) β 1 1 = lim β = β1. π‘β0 π‘ π‘+1
19. Rewriting the numerator as a single quotient we get 4 β (4 + β) 1 1 4 4+β ββ β = β = = 4+β 4 4(4 + β) 4(4 + β) 4(4 + β) 4(4 + β) provided β β 0. Thus lim
ββ0
1β(4 + β) β 1β4 1 ββ β1 = lim == lim =β . ββ0 4β(4 + β) ββ0 4(4 + β) β 16
1.9 SOLUTIONS 20. There are two ways to do this. One way is to multiply the numerator and denominator by
β
111
π§ + 1 and then simplify:
β β β ( π§)2 β 1 ( π§ β 1)( π§ + 1) 1 = = β β β (π§ β 1)( π§ + 1) (π§ β 1)( π§ + 1) π§+1 provided π§ β 1. Thus
β lim
A second way is to let π’ =
π§β1
π§β1
π§β1
1 1 = . = lim β π§β1 2 π§+1
β π§ so π§ = π’2 . Since π’ β 1 as π§ β 1, we can rewrite β lim π§β1
π§β1
π§β1
= lim
π’β1
.
π’β1 π’2 β 1
Factoring π’2 β 1 = (π’ β 1)(π’ + 1) and canceling the π’ β 1 factors since π’ β 1 in the limit, we get lim
π’β1
π’β1 π’2 β 1
= lim
1
π’β1 π’ + 1
=
1 . 2
β 21. There are two ways to do this. One way is to multiply the numerator and denominator by 9 + β + 3 and then simplify: (β ) (β ) 9+ββ3 9+β+3 9+ββ9 β 1 = (β (β ) ) = (β ) = β 9+β+3 β 9+β+3 β 9+β+3 β 9+β+3 provided β β 0. Thus
β lim
ββ0
A second way is to let π’ =
β
9+ββ3 1 1 = . = lim β ββ0 β 6 9+β+3
9 + β so β = π’2 β 9. Since π’ β 3 as β β 0, we can rewrite β 9+ββ3 π’β3 . = lim 2 lim ββ0 π’β3 π’ β 9 β
Factoring π’2 β 9 = (π’ β 3)(π’ + 3) and canceling the π’ β 3 factors since π’ β 3 in the limit, we get lim
π’β3
π’β3 π’2 β 9
= lim
1
π’β3 π’ + 3
=
1 . 6
22. There are two ways to do this. First, factoring the numerator and simplifying, we get (2π₯ )2 β 1 (2π₯ β 1)(2π₯ + 1) 4π₯ β 1 = π₯ = = 2π₯ + 1 π₯ 2 β1 2 β1 2π₯ β 1 provided π₯ β 0. Thus lim
4π₯ β 1
π₯β0 2π₯ β 1
= lim(2π₯ + 1) = 20 + 1 = 2. π₯β0
π₯
A second way is to let π’ = 2 . Since π’ β 1 as π₯ β 0, we can rewrite 4π₯ β 1 π’2 β 1 = lim . π₯ π₯β0 2 β 1 π’β1 π’ β 1
lim
Factoring π’2 β 1 = (π’ β 1)(π’ + 1) and canceling the π’ β 1 factors since π’ β 1 in the limit, we get π’2 β 1 = lim(π’ + 1) = 2. π’β1 π’ β 1 π’β1
lim
112
Chapter One /SOLUTIONS
23. Expanding the numerator, we get (1 + β)4 β 1 = 1 + 4β + 6β2 + 4β3 + β4 β 1. Next, factoring and simplifying, we get β(4 + 6β + 4β2 + β3 ) (1 + β)4 β 1 = = 4 + 6β + 4β2 + β3 β β provided β β 0. Thus
(1 + β)4 β 1 = lim(4 + 6β + 4β2 + β3 ) = 4. ββ0 ββ0 β lim
24. (a) We have π (4) = 7 and π(4) = 4β2 , so the limit is of the form 7β(4β2 ), not 0β0. (b) Since π (π₯)βπ(π₯) is continuous at π = 4, we have lim
π (π₯)
π₯β4 π(π₯)
=
π (4) 7 = β2 = 7 β 16 = 112. π(4) 4
25. (a) We have π (1) = 2(1)3 + (1)2 β 3(1) = 0 and π(1) = (1)2 + 3(1) β 4 = 0, so the limit is of the form 0β0. (b) Factoring, we have lim π₯β1
So lim π₯β1
π₯(2π₯2 + π₯ β 3) 2π₯3 + π₯2 β 3π₯ = lim π₯β1 (π₯ β 1)(π₯ + 4) π₯2 + 3π₯ β 4 π₯(2π₯ + 3)(π₯ β 1) = lim π₯β1 (π₯ β 1)(π₯ + 4) π₯(2π₯ + 3) = lim π₯β1 (π₯ + 4) (1)(2(1) + 3) 5 = = 1. = lim π₯β1 (1 + 4) 5
2π₯3 + π₯2 β 3π₯ = 1. π₯2 + 3π₯ β 4
26. (a) We have π (3) = (3)2 β 3(3) = 0 and π(3) = (b) Rationalizing the denominator, we have
β 3 + 1 β 2 = 0, so the limit is of the form 0β0.
β π₯+1+2 π₯2 β 3π₯ π₯2 β 3π₯ = lim β β β lim β π₯β3 π₯β3 π₯+1β2 π₯+1β2 π₯+1+2 β (π₯2 β 3π₯)( π₯ + 1 + 2) = lim π₯β3 (π₯ + 1) β 4 β π₯(π₯ β 3)( π₯ + 1 + 2) = lim π₯β3 (π₯ β 3) β = lim π₯( π₯ + 1 + 2) π₯β3 β = 3( 3 + 1 + 2) = 3(2 + 2) = 12. π₯2 β 3π₯ = 12. So lim β π₯β3 π₯+1β2 27. Dividing both numerator and denominator by π§3 , we get 5 + π§22 + π§13 0+0+0 5π§2 + 2π§ + 1 π§ = lim = = 0. π§ββ 2π§3 β π§2 + 9 π§ββ 2 β 1 + 9 2β0+0
lim
π§
π§3
28. Dividing both numerator and denominator by π₯2 , we get 1 + 7 β π₯112 7 π₯ + 7π₯2 β 11 π₯ = lim = . 2 π₯ββ π₯ββ 3 3π₯2 β 2π₯ 3β
lim
π₯
1.9 SOLUTIONS 29. Dividing both numerator and denominator by ππ‘ , we get 4 + π32π‘ 4 4ππ‘ + 3πβπ‘ = . = lim π‘ββ 5ππ‘ + 2π π‘ββ 5 + 2π 5 lim
ππ‘
30. We have,
( )π₯ 2π₯+1 2π₯ β 2 2 = lim = lim 6 =0 π₯ββ 3π₯β1 π₯ββ 3π₯ β 3β1 π₯ββ 3 π₯ since lim (2β3) = 0 because 2β3 < 1. lim
π₯ββ
31. We have,
23π₯+2 23π₯ β 22 = lim π₯ 3 = lim π₯+3 π₯ββ 3 π₯ββ 3 β 3 π₯ββ lim
( )π₯ 8 = β because 83 > 1. π₯ββ 3 32. We have,
( 3 )π₯ ( ) ( )π₯ ( ) 2 4 8 4 = lim = β, π₯ββ 3 3 27 27
since lim
lim π₯πβπ₯ = lim
π₯ββ π₯
since π grows faster than π₯.
π₯
π₯ββ ππ₯
33. We have,
= 0,
lim (4ππ‘ )(7πβπ‘ ) = lim
28ππ‘ = 28. ππ‘
lim π‘β2 sin π‘ = lim
sin π‘ = 0, π‘2
π‘ββ
π‘ββ
34. We have, π‘ββ
π‘ββ
since β1 β€ sin π‘ β€ 1 and π‘2 β β as π‘ β β. (β ) 35. First we use algebra: Multiply by 4 + β + 2 in numerator and denominator, then expand and simplify: β 4+ββ2=
(β
) (β ) 4+ββ2 4+β+2 β 4+ββ4 = β . = β (β ) 4+β+2 4+β+2 4+β+2
Now we can ο¬nd the limit: β lim
ββ0
36. First we combine the fractions:
4+ββ2 1 β 1 = . = lim (β ) = lim β ββ0 ββ0 β 4 4+β+2 β 4+β+2 β 2β 4+β 1 β = β . β 2 4+β 4+β 2 1
Now multiply by
(β ) 4 + β + 2 in numerator and denominator, then expand and simplify:
(
)( ) β β 2β 4+β 2+ 4+β 4 β (4 + β) ββ = β ( ) ( ) = β ( ). β β β β 2 4+β 2+ 4+β 2 4+β 2+ 4+β 2 4+β 2+ 4+β
Now we ο¬nd the limit: ( ) 1 1 1 ββ β1 1 β = lim β lim ( ) = lim β ( ) =β . β β β ββ0 β ββ0 ββ0 16 4+β 2 2β 4 + β 2 + 4 + β 2 4+β 2+ 4+β
113
114
Chapter One /SOLUTIONS
37. Given that β4π₯ + 6 β€ π (π₯) β€ π₯2 β 2π₯ + 7, we see that lim (β4π₯ + 6) β€ lim π (π₯) β€ lim (π₯2 β 2π₯ + 7)
π₯ββ1
π₯ββ1
π₯ββ1
β4(β1) + 6 β€ lim π (π₯) β€ (β1)2 β 2(β1) + 7 π₯ββ1
10 β€ lim π (π₯) β€ 10. π₯ββ1
Since 10 β€ lim π (π₯) β€ 10, we know that lim π (π₯) = 10. π₯ββ1
π₯ββ1
38. Given that 4 cos(2π₯) β€ π (π₯) β€ 3π₯2 + 4, we see that lim 4 cos(2π₯) β€ lim π (π₯) β€ lim(3π₯2 + 4) π₯β0
π₯β0
π₯β0
4 cos(0) β€ lim π (π₯) β€ 3(0)2 + 4 π₯β0
4 β€ lim π (π₯) β€ 4. π₯β0
Since 4 β€ lim π (π₯) β€ 4, we know that lim π (π₯) = 4. π₯β0
π₯β0
4π₯2 β 5 4π₯6 + 3 39. Given that β€ π (π₯) β€ , we see that π₯2 π₯6 4π₯2 β 5 4π₯6 + 3 β€ lim π (π₯) β€ lim 2 π₯ββ π₯ββ π₯ π₯6 4π₯2 5 4π₯6 3 lim β lim 2 β€ lim π (π₯) β€ lim 6 + lim 6 π₯ββ π₯2 π₯ββ π₯ π₯ββ π₯ββ π₯ π₯ββ π₯ (using the sum property since each limit exists) lim
π₯ββ
4 β 0 β€ lim π (π₯) β€ 4 + 0 π₯ββ
4 β€ lim π (π₯) β€ 4. π₯ββ
Since 4 β€ lim π (π₯) β€ 4, we know that lim π (π₯) = 4. π₯ββ
π₯ββ
PROBLEMS 40. Because the denominator equals 0 when π₯ = 4, so must the numerator. This means π2 = 16 and the choices for π are 4 or β4. 41. Because the denominator equals 0 when π₯ = 1, so must the numerator. So 1 β π + 4 = 0. The only possible value of π is 5. 42. Because the denominator equals 0 when π₯ = β2, so must the numerator. So 4 β 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 β 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 ππ β 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 π2 β 49 = 0 and the choices for π are 7 or β7. 46. Division of numerator and denominator by π₯2 yields 1 + 3βπ₯ + 5βπ₯2 π₯2 + 3π₯ + 5 = . π 4π₯ + 1 + π₯ 4βπ₯ + 1βπ₯2 + π₯πβ2 As π₯ β β, the limit of the numerator is 1. The limit of the denominator depends upon π. If π > 2, the denominator approaches β as π₯ β β, so the limit of the quotient is 0. If π = 2, the denominator approaches 1 as π₯ β β, so the limit of the quotient is 1. If π < 2 the denominator approaches 0+ as π₯ β β, so the limit of the quotient is β. Therefore the values of π we are looking for are π β₯ 2.
1.9 SOLUTIONS
115
) ) ( ( 47. For the numerator, lim π2π₯ β 5 = β5. If π > 0, lim πππ₯ + 3 = 3, so the quotient has a limit of β5β3. If π = 0, π₯βββ π₯βββ ) ( lim πππ₯ + 3 = 4, so the quotient has limit of β5β4. If π < 0, the limit of the quotient is given by lim (π2π₯ β5)β(πππ₯ +3) = π₯βββ
π₯βββ
0.
48. Division of numerator and denominator by π₯3 yields 1 β 6βπ₯3 π₯3 β 6 . = πβ3 π₯π + 3 π₯ + 3βπ₯3 As π₯ β β, the limit of the numerator is 1. The limit of the denominator depends upon π. If π > 3, the denominator approaches β as π₯ β β, so the limit of the quotient is 0. If π = 3, the denominator approaches 1 as π₯ β β, so the limit of the quotient is 1. If π < 3 the denominator approaches 0+ as π₯ β β, so the limit of the quotient is β. Therefore the values of π we are looking for are π β₯ 3. 49. We divide both the numerator and denominator by π5π₯ , giving π(πβ5)π₯ + 11βπ5π₯ πππ₯ + 11 = lim . π₯ββ π5π₯ β 3 π₯ββ 1 β 3βπ5π₯ lim
In the denominator, lim 1 β 3βπ5π₯ = 1. In the numerator, if π < 5, we have lim (π(πβ5)π₯ + 11βπ5π₯ ) = 0, so the quotient π₯ββ
π₯ββ
has a limit of 0. If π = 5, we have lim (π(πβ5)π₯ + 11βπ5π₯ ) = 1, so the quotient has a limit of 1. If π > 5, we have π₯ββ
lim (π(πβ5)π₯ + 11βπ5π₯ ) = β, so the limit of the quotient does not exist.
π₯ββ
50. We divide both the numerator and denominator by 32π₯ , giving 3(πβ2)π₯ + 6β32π₯ 3ππ₯ + 6 = . 2π₯ π₯ββ 3 + 4 1 + 4β32π₯ lim
In the denominator, lim 1+4β32π₯ = 1. In the numerator, if π < 2, we have lim 3(πβ2)π₯ +6β32π₯ = 0, so the quotient has a limit π₯ββ
π₯ββ
of 0. If π = 2, we have lim 3(πβ2)π₯ + 6β32π₯ = 1, so the quotient has a limit of 1. If π > 2, we have lim 3(πβ2)π₯ + 6β32π₯ = β, π₯ββ π₯ββ so the quotient has a limit of β. 51. In the denominator, we have lim 32π₯ + 4 = 4. In the numerator, if π < 0, we have lim 3ππ₯ + 6 = β, so the quotient has π₯βββ
π₯βββ
a limit of β. If π = 0, we have lim 3ππ₯ + 6 = 7, so the quotient has a limit of 7β4. If π > 0, we have lim 3ππ₯ + 6 = 6, π₯βββ
π₯βββ
so the quotient has a limit of 6β4. β 52. Let π‘ = π¦ so that π¦ = π‘2 . Since π‘ β 2 as π¦ β 4, we have lim π¦β4
53. Let π‘ =
β
β π¦β2 π¦β4
π‘β2 = lim 2 π‘β2 π‘ β 4 π‘β2 = lim π‘β2 (π‘ β 2)(π‘ + 2) 1 = lim π‘β2 π‘ + 2 1 = . 4
π₯ so that π₯ = π‘2 . Since π‘ β 3 as π₯ β 9, we have β π₯β π₯β6 π‘2 β π‘ β 6 = lim lim β π₯β9 π‘β3 π‘β3 π₯β3 (π‘ β 3)(π‘ + 2) = lim π‘β3 π‘β3 = lim(π‘ + 2) π‘β3
= 5.
116
Chapter One /SOLUTIONS
54. Let π‘ =
β
1 + β so that π‘2 = 1 + β and β = π‘2 β 1. Since π‘ β 1 as β β 0, we have β 1+ββ1 π‘β1 lim = lim 2 ββ0 π‘β1 π‘ β 1 β π‘β1 = lim π‘β1 (π‘ β 1)(π‘ + 1) 1 = lim π‘β1 π‘ + 1 1 = . 2
β 55. Let π‘ = 3 π₯ so that π₯ = π‘3 . Since π‘ β 1 as π₯ β 1, we have β 3 π₯β1 π‘β1 lim = lim 3 π₯β1 π₯ β 1 π‘β1 π‘ β 1 = lim
π‘β1
π‘β1 (π‘ β 1)(π‘2 + π‘ + 1)
1 = lim 2 π‘β1 π‘ + π‘ + 1 1 = . 3 56. Let π‘ = ππ₯ so that π3π₯ = (ππ₯ )3 = π‘3 and π2π₯ = π‘2 . Since π‘ β 1 as π₯ β 0, we have π3π₯ β π2π₯ π‘3 β π‘2 = lim π₯ π₯β0 π β 1 π‘β1 π‘ β 1 π‘2 (π‘ β 1) = lim π‘β1 π‘β1 = lim π‘2
lim
π‘β1
= 1. 57. Let π‘ = ππ₯ so that π3π₯ = (ππ₯ )3 = π‘3 . Since π‘ β β as π₯ β β, we have: lim
2π3π₯ β 1
π₯ββ 5π3π₯ + ππ₯ + 1
= lim
2π‘3 β 1
π‘ββ 5π‘3 + π‘ + 1
2 β 1βπ‘3 Dividing numerator and denominator by π‘3 π‘ββ 5 + π‘βπ‘3 + 1βπ‘3 2 β 1βπ‘3 = lim Simplifying π‘ββ 5 + 1βπ‘2 + 1βπ‘3 2β0 2 = Since 1βπ‘2 β 0 and 1βπ‘3 β 0 as π‘ β β = . 5+0+0 5 = lim
1 sin π₯ 1 β€ β€ . Since π₯ π₯ π₯ 1 1 lim β = 0 = lim , π₯ββ π₯ π₯ββ π₯
58. We know that β1 β€ sin π₯ β€ 1. If we divide by π₯, π₯ β 0, we get β
we know that lim
π₯ββ
sin π₯ = 0. π₯
59. For π₯ β₯ 0, since 0 < πβπ₯ β€ 1, we have π₯ < π₯ + πβπ₯ < π₯ + 1. Therefore, lim
1
π₯ββ π₯ + 1
= 0 = lim
1
π₯ββ π₯
, we have lim
1
π₯ββ π₯ + 1
β€ lim
1
π₯ββ π₯ + πβπ₯
0 β€ lim
1
π₯ββ π₯ + πβπ₯
β€ lim
1
π₯ββ π₯
β€0
1 1 1 < . Therefore, since < π₯+1 π₯ + πβπ₯ π₯
1.9 SOLUTIONS 1
Thus, lim
π₯ββ π₯ + πβπ₯
= 0.
60. For all π₯, we know that β1 β€ cos π₯ β€ 1, and hence that 0 β€ cos2 π₯ β€ 1. It follows that 1 cos2 π₯ β€ . 2π₯ + 1 2π₯ + 1
0β€ Therefore, since lim 0 = 0 and lim
1
π₯ββ 2π₯ + 1
π₯ββ
= 0, we have lim
cos2 π₯
π₯ββ 2π₯ + 1
= 0 by the Squeeze Theorem.
61. For all π₯ β 0, we know that β1 β€ sin(1βπ₯) β€ 1. It follows that βπ₯4 β€ π₯4 sin(1βπ₯) β€ π₯4 . Therefore, since lim(βπ₯4 ) = 0 and lim π₯4 = 0, we have lim π₯4 sin(1βπ₯) = 0 by the Squeeze Theorem. π₯β0
π₯β0
π₯β0
62. For all π₯ β₯ 0, we know that
π₯ 1 π₯ 0β€ β β€ β = β . 3 3 π₯ π₯ +1 π₯ 1 π₯ Therefore, since lim 0 = 0 and lim β = 0, we have lim β = 0 by the Squeeze Theorem. π₯ββ π₯ββ π₯ββ π₯ π₯3 + 1 63. We know that β1 β€ cos π₯ β€ 1, and hence that 0 β€ 2 cos2 π₯ β€ 2. Therefore, π₯ β€ π₯ + 2 cos2 π₯ β€ π₯ + 2, so for π₯ > 0, 1 1 1 β€ . β€ π₯+2 π₯ π₯ + 2 cos2 π₯ 1
Since lim
π₯ββ π₯ + 2
64. Since π₯2 sin
( ) 1 π₯
= 0 and lim
1
π₯ββ π₯
1
= 0, we have lim
π₯ββ π₯ + 2 cos2 π₯
= 0 by the Squeeze Theorem.
+ 1 is squeezed between π¦ = π₯2 + 1 and π¦ = βπ₯2 + 1, ) ( ( ) 1 + 1 = lim(π₯2 + 1) = lim(βπ₯2 + 1) = 1. lim π₯2 sin π₯β0 π₯β0 π₯β0 π₯
See Figure 1.127. π¦ π¦ = π₯2 + 1 π¦ = π₯2 sin
( ) 1 π₯
+1
π¦ = βπ₯2 + 1 π₯
Figure 1.127
65. Since sin
( ) 1 π₯
+ 2 is oscillates between π¦ = 3 and π¦ = 1, the limit as π₯ β 0 does not exist. See Figure 1.128. π¦ π¦=3 ( ) π¦ = sin π₯1 + 2 π¦=1 π₯
Figure 1.128
117
118
Chapter One /SOLUTIONS
66. There are many possible correct answers. (a) If π (π₯) = 1βπ₯2 and π(π₯) = 1βπ₯ then π (π₯)βπ(π₯) = 1βπ₯ so lim
π (π₯)
π₯ββ π(π₯)
= 0.
π (π₯) = 1. (b) If π (π₯) = 1βπ₯ and π(π₯) = 1βπ₯ then π (π₯)βπ(π₯) = 1 so lim π₯ββ π(π₯) π (π₯) = β. (c) If π (π₯) = 1βπ₯ and π(π₯) = 1βπ₯2 then π (π₯)βπ(π₯) = π₯ so lim π₯ββ π(π₯) 67. There are many possible choices for π(π₯). One possibility is π(π₯) =
(
) ( ) π₯3 β 3π₯2 + π₯ β 3 π₯β3 π₯β3 β π (π₯) = (π₯2 + 1) = . π₯β3 π₯β3 π₯β3
Observe that π (π₯) = π(π₯) wherever π (π₯) is deο¬ned except for π₯ = 3 since π(3) is undeο¬ned. This means the graphs of π (π₯) and π(π₯) will be the same except at π₯ = 3 where the graph of π(π₯) has a hole. Since the graphs of π (π₯) and π(π₯) are identical except at π₯ = 3, the hole will have the same coordinates as the function π (π₯) at π₯ = 3, so the coordinates of the hole will be (3, 10). 68. There are many possible choices for π(π₯). One possibility is π(π₯) =
( ) ( ) π₯3 + π₯ π₯ π₯ β π (π₯) = (π₯2 + 1) = . π₯ π₯ π₯
Observe that π (π₯) = π(π₯) wherever π (π₯) is deο¬ned except for π₯ = 0 since π(0) is undeο¬ned. This means the graphs of π (π₯) and π(π₯) will be the same except at π₯ = 0 where the graph of π(π₯) has a hole. Since the graphs of π (π₯) and π(π₯) are identical except at π₯ = 0, the hole will have the same coordinates as the function π (π₯) at π₯ = 0, so the coordinates of the hole will be (0, 1). 69. There are many possible choices for π(π₯). One possibility is ) ( ) ( π₯ ln π₯ β ln π₯ π₯β1 π₯β1 β π (π₯) = ln π₯ = . π(π₯) = π₯β1 π₯β1 π₯β1 Observe that π (π₯) = π(π₯) wherever π (π₯) is deο¬ned except for π₯ = 1 since π(1) is undeο¬ned. This means the graphs of π (π₯) and π(π₯) will be the same except at π₯ = 1 where the graph of π(π₯) has a hole. Since the graphs of π (π₯) and π(π₯) are identical except at π₯ = 1, the hole will have the same coordinates as the function π (π₯) at π₯ = 1, so the coordinates of the hole will be (1, 0). 70. There are many possible choices for π(π₯). One possibility is ) ( ) ( π₯ sin π₯ β π sin π₯ π₯βπ π₯βπ β π (π₯) = sin π₯ = . π(π₯) = π₯βπ π₯βπ π₯βπ Observe that π (π₯) = π(π₯) wherever π (π₯) is deο¬ned except for π₯ = π since π(π) is undeο¬ned. This means the graphs of π (π₯) and π(π₯) will be the same except at π₯ = π where the graph of π(π₯) has a hole. Since the graphs of π (π₯) and π(π₯) are identical except at π₯ = π, the hole will have the same coordinates as the function π (π₯) at π₯ = π, so the coordinates of the hole will be (π, 0). 71. We have (π₯ β 1)3 π₯β1 (π₯ β 1)2 = lim(π₯ β 1)
Cancelling (π₯ β 1) since π₯ β 1
= 1 β 1 = 0.
Substituting π₯ = 1 since (π₯ β 1) is continuous
lim π (π₯) = lim π₯β1
π₯β1
72. We have (π₯ β 1)2 π₯β1 (π₯ β 1)3 1 = lim π₯β1 (π₯ β 1)
lim π (π₯) = lim π₯β1
Cancelling (π₯ β 1)2 since π₯ β 1
So the function π (π₯) takes the same values as 1β(π₯ β 1) except at π₯ = 1, so it must have the same limit. Since the limit of the denominator of 1β(π₯ β 1) is 0 and the numerator is 1 at π₯ = 1, this limit does not exist.
1.9 SOLUTIONS
119
73. We have (π₯ β 1)2 π₯β1 (π₯ β 1)2 = lim(1) Cancelling (π₯ β 1)2 since π₯ β 1
lim π (π₯) = lim π₯β1
π₯β1
= 1. 74. We have lim π (π₯) = lim π₯β1
(π₯ β 1)π
π₯β1 (π₯ β 1)π
= lim(π₯ β 1)πβπ
Cancelling (π₯ β 1)π since π₯ β 1 and π > π
π₯β1
= (1 β 1)πβπ = 0.
Substituting π₯ = 1 since (π₯ β 1)πβπ is continuous
75. We have (π₯ β 1)π π₯β1 (π₯ β 1)π 1 = lim π₯β1 (π₯ β 1)πβπ
lim π (π₯) = lim π₯β1
Cancelling (π₯ β 1)π since π₯ β 1 and π > π
So the function π (π₯) takes the same values as 1β(π₯ β 1)πβπ except at π₯ = 1, so it must have the same limit. Since the limit of the denominator of 1β(π₯ β 1)πβπ is 0 and the numerator is 1 at π₯ = 1, this limit does not exist. 76. Since π = π, we have lim π (π₯) = lim π₯β1
(π₯ β 1)π
π₯β1 (π₯ β 1)π
= lim(1)
Cancelling (π₯ β 1)π since π₯ β 1
π₯β1
= 1. 1 1 1 1 = 0 = lim and lim β = 0 = lim . π₯ββ π₯ π₯βββ π₯ π₯βββ π₯ π₯ In both cases πΏ = 0. The Squeeze Theorem cannot be applied to other cases since for any other π,
77. The Squeeze Theorem can be applied when π = β or π = ββ since lim β π₯ββ
lim β π₯βπ
1 1 1 1 = β β = lim . π₯ π π π₯βπ π₯
Strengthen Your Understanding 78. If we factor the numerator of π and simplify, we see that π (π₯) = π₯ β 1, for π₯ β β1. This show that the two functions are identical (that is, have the same values) where they are both deο¬ned, the functions have diο¬erent domains: π₯ = β1 is in the domain of π but not in the domain of π . 79. The limit lim π (π₯)βπ(π₯) depends on the values of π (π₯)βπ(π₯) as π₯ approaches 1 but is not necessarily dependent on the π₯β1
value at π₯ = 1. For example, we can take π(π₯) = 1 and { π (π₯) =
β1 0 1
π₯<1 π₯=1 . 1<π₯
For these choices of π (π₯) and π(π₯), we have π (1) = 0 and π(1) = 1 as required. However, for all π₯ < 1, π (π₯)βπ(π₯) = β1 so limβ π (π₯)βπ(π₯) = β1, and for π₯ > 1, π (π₯)βπ(π₯) = 1, so lim+ π (π₯)βπ(π₯) = 1. Thus the one sided limits are diο¬erent, so π₯β1
lim π (π₯)βπ(π₯) does not exist.
π₯β1
π₯β1
80. False, since the limit lim π (π₯) may not even exist. For example if π(π₯) = β1, π(π₯) = 1 and π (π₯) = sin(1βπ₯), then the π₯β0
conditions are met but sin(1βπ₯) has no limit as π₯ β 0. 81. True, by the Squeeze Theorem, using the constant function π(π₯) = 0.
120
Chapter One /SOLUTIONS
82. False, this is a confused, and incorrect, version of the Squeeze Theorem. For example if π(π₯) = π (π₯) = π₯, and π(π₯) = 1 then the conditions are met but lim π (π₯) = 0 and lim π(π₯) = 1. π₯β0
π₯β0
83. False, for example if π (π₯) = 0, and π(π₯) = π₯ then the conditions are met but lim
π (π₯)
π₯β0 π(π₯)
84. False, for example if π (π₯) = 1, and π(π₯) = π₯ then the conditions are met but lim and limβ π₯β0
π (π₯)
π₯β0 π(π₯)
1 = ββ. π₯
85. False, for example if π (π₯) = 1βπ₯, and π(π₯) = 1βπ₯2 then lim
π (π₯)
π₯β0 π(π₯)
= 0. does not exist, since lim+ π₯β0
1 =β π₯
= lim π₯ = 0 but the limits of π (π₯) and π(π₯) do not exist, π₯β0
1 1 1 since lim+ = β (and limβ = ββ) and lim 2 = β. π₯β0 π₯ π₯β0 π₯ π₯β0 π₯ 86. True, this follows from the multiplicative limit property: if lim π(π₯) exists and lim π(π₯) exists then lim π(π₯) β π(π₯) exists (using π(π₯) = π (π₯)βπ(π₯) and π(π₯) = π(π₯)).
π₯β0
π₯β0
π₯β0
87. False, for example if π(π₯) = 1 when π₯ > 0 and π(π₯) = β1 when π₯ < 0, then setting π (π₯) = π(π₯), π (π₯) and using π = 0 gives lim = lim 1 = 1. π₯β0 π(π₯) π₯β0
Solutions for Section 1.10 EXERCISES 1. For each πΏ we determine whether the graph of π (π₯) on the interval 3 β πΏ < π₯ < 3 + πΏ stays in the shaded region πΏ β π < π¦ < πΏ + π in the ο¬gure. Notice that as πΏ gets smaller, the interval gets shorter. (a) No for πΏ = 1. The graph of π (π₯) on the interval 2 < π₯ < 4 extends outside the shaded region. (b) No for πΏ = 0.75. The graph of π (π₯) on the interval 2.25 < π₯ < 3.75 extends outside the shaded region. (c) Yes for πΏ = 0.5. The graph of π (π₯) on the interval 2.5 < π₯ < 3.5 ο¬ts inside the shaded region. (d) Yes for πΏ = 0.25. The graph of π (π₯) on the interval 2.75 < π₯ < 3.25 ο¬ts inside the shaded region. (e) Yes for πΏ = 0.1. The graph of π (π₯) on the interval 2.9 < π₯ < 3.1 ο¬ts inside the shaded region. 2. For each πΏ we determine whether the graph of π(π₯) on the interval 20 β πΏ < π₯ < 20 + πΏ stays in the shaded region πΏ β π < π¦ < πΏ + π in the ο¬gure. Notice that as πΏ gets smaller, the interval gets shorter. (a) No for πΏ = 0.5. The graph of π(π₯) on the interval 19.5 < π₯ < 20.5 extends outside the shaded region. (b) No for πΏ = 0.4. The graph of ππ₯) on the interval 19.6 < π₯ < 20.4 extends outside the shaded region. (c) No for πΏ = 0.3. The graph of π(π₯) on the interval 19.7 < π₯ < 20.3 extends outside the shaded region. (d) Yes for πΏ = 0.2. The graph of π(π₯) on the interval 19.8 < π₯ < 20.2 ο¬ts inside the shaded region. (e) Yes for πΏ = 0.1. The graph of π(π₯) on the interval 19.9 < π₯ < 20.1 ο¬ts inside the shaded region. 3. By tracing on a calculator or solving equations, we ο¬nd the following values of πΏ: For π = 0.2, πΏ β€ 0.1. For π = 0.1, πΏ β€ 0.05. For π = 0.02, πΏ β€ 0.01. For π = 0.01, πΏ β€ 0.005. For π = 0.002, πΏ β€ 0.001. For π = 0.001, πΏ β€ 0.0005. 4. By tracing on a calculator or solving equations, we ο¬nd the following values of πΏ: For π = 0.1, πΏ β€ 0.46. For π = 0.01, πΏ β€ 0.21. For π = 0.001, πΏ < 0.1. Thus, we can take πΏ β€ 0.09. 5. Since |4π₯ β 12| = 4|π₯ β 3|, to get |4π₯ β 12| < 0.1 we require that |π₯ β 3| < 0.1β4 = 0.025. Thus we take πΏ = 0.025. 6. Since |(2π₯ β 2) β 0| = 2|π₯ β 1|, to get |(2π₯ β 2) β 0| < 0.1 we require that |π₯ β 1| < 0.1β2 = 0.05. Thus we take πΏ = 0.05. 7. Since |(5π₯ + 3) β (β7)| = |5π₯ + 10| = 5|π₯ + 2|, to get |(5π₯ + 3) β (β7)| < 0.1 we require that |π₯ + 2| < 0.1β5 = 0.02. Thus we take πΏ = 0.02. β 8. Since |(π₯2 + 2) β 2| = |π₯2 | = |π₯|2 , to get |(π₯2 + 2) β 2| < 0.1 we require that |π₯| < 0.1 = 0.316. Thus we take πΏ = 0.316.
1.10 SOLUTIONS
121
PROBLEMS 9. The statement
lim π(β) = πΎ
ββπ
means that we can make the value of π(β) as close to πΎ as we want by choosing β suο¬ciently close to, but not equal to, π. In symbols, for any π > 0, there is a πΏ > 0 such that |π(β) β πΎ| < π
for all 0 < |β β π| < πΏ.
10. By tracing on a calculator or solving equations, we ο¬nd the following values of πΏ: For π = 0.1, πΏ β€ 0.1 For π = 0.05, πΏ β€ 0.05. For π = 0.0007, πΏ β€ 0.00007. 11. By tracing on a calculator or solving equations, we ο¬nd the following values of πΏ: For π = 0.1, πΏ β€ 0.45. For π = 0.001, πΏ β€ 0.0447. For π = 0.00001, πΏ β€ 0.00447. 12. We want to ο¬nd πΏ > 0 such that if βπΏ < π₯ < πΏ, then |ππ₯ β 1| < 0.1. Observe that |ππ₯ β 1| < 0.1 β0.1 < ππ₯ β 1 < 0.1 ln(0.9) < π₯ < ln(1.1), and that ln(0.9) = β0.105 and ln(1.1) = 0.095. We therefore choose πΏ = ln(1.1) so that βπΏ < π₯ < πΏ implies ln(0.9) < β ln(1.1) < π₯ < ln(1.1), π₯
which, in turn, implies that |π β 1| < 0.1 (see Figure 1.129). π¦ = 0.1
π¦ = β0.1 π₯ = β ln(1.1)
π₯ = ln(1.1) π₯
Figure 1.129: Graph of π β 1 with β ln(1.1) < π₯ < ln(1.1) 13. We want to ο¬nd πΏ > 0 such that if βπΏ < π₯ β 1 < πΏ, then | ln π₯| < 0.1. Observe that | ln π₯| < 0.1 β0.1 < ln π₯ < 0.1 πβ0.1 < π₯ < π0.1 β0.1
π
β 1 < π₯ β 1 < π0.1 β 1
and that 1 β πβ0.1 = 0.095 and π0.1 β 1 = 0.105. We therefore choose πΏ = 1 β πβ0.1 so that βπΏ < π₯ β 1 < πΏ implies πβ0.1 β 1 < π₯ β 1 < 1 β πβ0.1 < π0.1 β 1, which, in turn, implies that | ln π₯| < 0.1 (see Figure 1.130).
122
Chapter One /SOLUTIONS π¦ = 0.1
π¦ = β0.1 π₯=1βπΏ
π₯=1+πΏ
Figure 1.130: Graph of ln π₯ with 1 β πΏ < π₯ < 1 + πΏ, where πΏ = 1 β πβ0.1 . 14. We want to ο¬nd πΏ > 0 such that if βπΏ < π₯ β 1 < πΏ, then | arctan π₯ β (πβ4)| < 0.1. Observe that | | |arctan π₯ β π | < 0.1 | 4 || | π β0.1 < arctan π₯ β < 0.1 4 π π β 0.1 < arctan π₯ < + 0.1 4 4 ) ( ) ( π π β 0.1 < π₯ < tan + 0.1 tan 4 4 ) ( ) ( π π β 0.1 β 1 < π₯ β 1 < tan + 0.1 β 1, tan 4 4 and that 1 β tan((πβ4) β 0.1) = 0.182 and tan((πβ4) + 0.1) β 1 = 0.223. We therefore choose πΏ = 1 β tan((πβ4) β 0.1) so that βπΏ < π₯ β 1 < πΏ implies ) ( ) ( ) ( π π π β 0.1 β 1 < π₯ β 1 < 1 β tan β 0.1 < tan + 0.1 β 1, tan 4 4 4 which, in turn, implies that | arctan π₯ β (πβ4)| < 0.1 (see Figure 1.131). π¦ = π4 + 0.1
π¦ = π4 β 0.1 π₯=1βπΏ
π₯=1+πΏ
Figure 1.131: Graph of arctan π₯ with 1 β πΏ < π₯ < 1 + πΏ, where πΏ = 1 β tan((πβ4) β 0.01). 15. We want to ο¬nd πΏ > 0 such that if βπΏ < π₯ β 2 < πΏ, then |(1βπ₯) β (1β2)| < 0.1. Observe that |1 1| | β | < 0.1 |π₯ 2| | | 1 1 1 β 0.1 < < + 0.1 2 π₯ 2 1 3 2 < < 5 π₯ 5 5 5 <π₯< 3 2 1 1 β <π₯β2 < . 3 2
1.10 SOLUTIONS
123
We therefore choose πΏ = 1β3 so that βπΏ < π₯ β 2 < πΏ implies 1 1 1 <π₯β2< < , 3 3 2 which, in turn, implies that |(1βπ₯) β (1β2)| < 0.1 (see Figure 1.132). β
π¦ = 12 + 0.1
π¦ = 12 β 0.1 π₯ = 5β3
π₯ = 7β3
Figure 1.132: Graph of 1βπ₯ with 5β3 < π₯ < 7β3. β 16. We want to ο¬nd πΏ > 0 such that if βπΏ < π₯ β 4 < πΏ, then | π₯ β 2| < 0.1. Observe that β | π₯ β 2| < 0.1 β 1.9 < π₯ < 2.1 3.61 < π₯ < 4.41 β0.39 < π₯ β 4 < 0.41. We therefore choose πΏ = 0.39 so that βπΏ < π₯ β 4 < πΏ implies β0.39 < π₯ β 4 < 0.39 < 0.41, β which, in turn, implies that | π₯ β 2| < 0.1 (see Figure 1.133). π¦ = 2 + 0.1
π¦ = 2 β 0.1 π₯ = β0.39
π₯ = 0.39
β Figure 1.133: Graph of π₯ with β0.39 < π₯ < 0.39.
17. From Table 1.17, it appears the limit is 0. This is conο¬rmed by Figure 1.134. An appropriate window is β0.015 < π₯ < 0.015, β0.01 < π¦ < 0.01. 0.01
Table 1.17 π₯
π (π₯)
π₯
π (π₯)
0.1
0.0666
β0.0001
β0.0001
0.01
0.0067
β0.001
β0.0007
0.001
0.0007
β0.01
β0.0067
0.0001
0.0001
β0.1
β0.0666
β0.01 β0.015
Figure 1.134
0.015
124
Chapter One /SOLUTIONS
18. From Table 1.18, it appears the limit is 0. This is conο¬rmed by Figure 1.135. An appropriate window is β0.0029 < π₯ < 0.0029, β0.01 < π¦ < 0.01. 0.01
Table 1.18 π₯
π (π₯)
π₯
π (π₯)
0.1
0.3365
β0.0001
β0.0004
0.01
0.0337
β0.001
β0.0034
0.001
0.0034
β0.01
β0.0337
0.0001
0.0004
β0.1
β0.3365
β0.01 β0.0029
0.0029
Figure 1.135
19. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯ β 2| < πΏ with π₯ β 2, then |(5π₯ β 6) β 4| < π. Observe that |(5π₯ β 6) β 4| = |5π₯ β 10| = 5|π₯ β 2|. Choose πΏ = πβ5. If |π₯ β 2| < πΏ with π₯ β 2, we have |(5π₯ β 6) β 4| = 5|π₯ β 2| < 5πΏ = π, proving that lim (5π₯ β 6) = 4. π₯β2
20. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯ + 1| < πΏ with π₯ β β1, then |(3π₯ + 1) + 2| < π. Observe that |(3π₯ + 1) + 2| = |3π₯ + 3| = 3|π₯ + 1|. Choose πΏ = πβ3. If |π₯ + 1| < πΏ with π₯ β β1, we have |(3π₯ + 1) + 2| = 3|π₯ + 1| < 3πΏ = π, proving that lim (3π₯ + 1) = β2. π₯ββ1
21. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯| < πΏ with π₯ β 0, then |(β2π₯ + 3) β 3| < π. Observe that |(β2π₯ + 3) β 3| = | β 2π₯| = 2|π₯|. Choose πΏ = πβ2. If |π₯| < πΏ with π₯ β 0, we have |(β2π₯ + 3) β 3| = 2|π₯| < 2πΏ = π, proving that lim (β2π₯ + 3) = 3. π₯β0
22. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯| < πΏ with π₯ β 0, then |(π₯2 + 2) β 2| < π. Observe that |(π₯2 + 2) β 2| = |π₯2 | = |π₯|2 . Choose πΏ =
β
π. If |π₯| < πΏ with π₯ β 0, we have |(π₯2 + 2) β 2| = |π₯|2 < πΏ 2 = π,
proving that lim (π₯2 + 2) = 2. π₯β0
23. For any π > 0, we want to ο¬nd the πΏ such that | | | | |π(π₯) β 2| = |βπ₯3 + 2 β 2| = |π₯3 | < π. | | | | Choose πΏ = π 1β3 . Then if |π₯| < πΏ = π 1β3 , it follows that |π(π₯) β 2| = ||π₯3 || < π.
1.10 SOLUTIONS
125
24. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯ β 1| < πΏ with π₯ β β1, then | | 2π₯2 + π₯ β 3 | β 5|| < π. | π₯β1 | | Observe that, if π₯ β 1, then | | (2π₯ + 3)(π₯ β 1) | | 2π₯2 + π₯ β 3 | β 5|| = || β 5|| = |2π₯ + 3 β 5| = 2|π₯ β 1|. | π₯β1 π₯ β 1 | | | | Choose πΏ = πβ2. If |π₯ β 1| < πΏ with π₯ β 1, we have | 2π₯2 + π₯ β 3 | | β 5|| = 2|π₯ β 1| < 2πΏ = π, | π₯β1 | | 2π₯2 + π₯ β 3 = 5. π₯β1 25. For any π > 0, we must show that there exists πΏ > 0 such that, if |π₯ + 3| < πΏ with π₯ β β3, then proving that lim π₯β1
| | π₯2 + 2π₯ β 3 | + 4|| < π. | π₯+3 | | Observe that, if π₯ β β3, then | | (π₯ + 3)(π₯ β 1) | | π₯2 + 2π₯ β 3 | + 4|| = || + 4|| = |π₯ + 3|. | π₯+3 π₯ + 3 | | | | Choose πΏ = π. If |π₯ + 3| < πΏ with π₯ β β3, we have | | π₯2 + 2π₯ β 3 | + 4|| = |π₯ + 3| < πΏ = π, | π₯+3 | | π₯2 + 2π₯ β 3 = β4. 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 π (π₯) is not close to 1. By choosing values of π₯ for which π (π₯) = 0, we see that |π (π₯) β 1| = 1; that is, the distance between π (π₯) and 1 equals 1. For any nonzero integer π, we have proving that lim
π₯ββ3
π (π₯) = 0 sin(1βπ₯) = 0 1 = ππ π₯ 1 , π₯= ππ so π (1β(ππ)) = 0. Choose π to be any real number less than one, and consider any πΏ > 0. Then we can choose a positive integer π large enough so that, if π₯ = 1β(ππ), then |π₯| < πΏ. Thus, π₯ is close to 0, but π (π₯) = 0 is not close to 1 because |π (π₯) β 1| = 1 > π (see Figure 1.136). This proves that lim π (π₯) β 1. π₯β0
π¦ 1+π 1 1βπ 1 ππ
πΏ
Figure 1.136
π (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 π (π₯) is not close to πΏ. By choosing values of π₯ for which π (π₯) = 1, we see that |π (π₯) β πΏ| = |1 β πΏ|; that is, the distance between π (π₯) and πΏ equals |1 β πΏ| > 0. Observe that π (π₯) = 1 sin(1βπ₯) = 1 π 5π 9π 13π 1 = , , , ,β¦ π₯ 2 2 2 2 2 2 2 2 , , ,β―, π₯= , π 5π 9π 13π so π (π₯) = 0 if π₯ = 2β((4π β 3)π) for a positive integer π. Choose π = |1 β πΏ|β2, and consider any πΏ > 0. Then we can choose a positive integer π large enough so that, if π₯ = 2β((4π β 3)π), then |π₯| < πΏ. Thus, π₯ is close to 0, but π (π₯) = 1 is not close to πΏ because |π (π₯) β πΏ| = |1 β πΏ| > π (see Figure 1.137). This proves that lim π (π₯) β πΏ. π₯β0
π¦ 1
π (π₯)
πΏ+π
2 (4πβ3)π
πΏ πΏ
πΏβπ
π₯
Figure 1.137 27. (a) For any π, we have π (π) = π. This means |π (π₯) β π (π)| = |π β π| = 0 for any π₯ and π. So given π > 0, choose any πΏ, for example πΏ = 1. Then |π₯ β π| < πΏ implies |π (π₯) β π (π)| = 0 < π. So lim π (π₯) = π (π), so π is continuous π₯βπ everywhere. (b) Given any π > 0, we can take πΏ = π, so that when |π₯ β π| < πΏ, |π(π₯) β π(π)| = |π₯ β π| < π. So, lim π(π₯) = π(π) and π π₯βπ is continuous everywhere. 28. The only change is that, instead of considering all π₯ near π, we only consider π₯ near to and greater than π. Thus the phrase β|π₯ β π| < πΏβ must be replaced by βπ < π₯ < π + πΏ.β Thus, we deο¬ne lim π (π₯) = πΏ
π₯βπ +
to mean that for any π > 0 (as small as we want), there is a πΏ > 0 (suο¬ciently small) such that if π < π₯ < π + πΏ, then |π (π₯) β πΏ| < π. 29. The only change is that, instead of considering all π₯ near π, we only consider π₯ near to and less than π. Thus the phrase β|π₯ β π| < πΏβ must be replaced by βπ β πΏ < π₯ < π.β Thus, we deο¬ne lim π (π₯) = πΏ
π₯βπ β
to mean that for any π > 0 (as small as we want), there is a πΏ > 0 (suο¬ciently small) such that if π β πΏ < π₯ < π, then |π (π₯) β πΏ| < π. 30. Instead of being βsuο¬ciently close to π,β we want π₯ to be βsuο¬ciently large.β Using π to measure how large π₯ must be, we deο¬ne lim π (π₯) = πΏ π₯ββ
to mean that for any π > 0 (as small as we want), there is a π > 0 (suο¬ciently large) such that if π₯ > π, then |π (π₯)βπΏ| < π. 31. (a) If π = 0, then the property says limπ₯βπ 0 = 0, which is easy to see is true. π , then multiplying by |π| gives (b) If |π (π₯) β πΏ| < |π| |π||π (π₯) β πΏ| < π. Since |π||π (π₯) β πΏ| = |π(π (π₯) β πΏ)| = |ππ (π₯) β ππΏ|, we have |ππ (π₯) β ππΏ| < π.
1.10 SOLUTIONS
127
(c) Suppose that lim π (π₯) = πΏ. We want to show that lim ππ (π₯) = ππΏ. If we are to have π₯βπ
π₯βπ
|ππ (π₯) β ππΏ| < π, then we will need |π (π₯) β πΏ| < We choose πΏ small enough that |π₯ β π| < πΏ
implies
π . |π|
|π (π₯) β πΏ| <
π . |π|
By part (b), this ensures that |ππ (π₯) β ππΏ| < π, as we wanted. 32. Suppose lim π (π₯) = πΏ1 and lim π(π₯) = πΏ2 . Then we need to show that π₯βπ
π₯βπ
lim (π (π₯) + π(π₯)) = πΏ1 + πΏ2 . π₯βπ
Let π > 0 be given. We need to show that we can choose πΏ > 0 so that whenever |π₯ β π| < πΏ, we will have |(π (π₯) + π(π₯)) β (πΏ1 + πΏ2 )| < π. First choose πΏ1 > 0 so that |π₯ β π| < πΏ1 implies |π (π₯) β πΏ1 | < π ; we can do this since | | 2 lim π (π₯) = πΏ1 . Similarly, choose πΏ2 > 0 so that |π₯ β π| < πΏ2 implies |π(π₯) β πΏ2 | < 2π . Now, set πΏ equal to the smaller of π₯βπ
πΏ1 and πΏ2 . Thus |π₯ β π| < πΏ will make both |π₯ β π| < πΏ1 and |π₯ β π| < πΏ2 . Then, for |π₯ β π| < πΏ, we have ) ( ) ( |π (π₯) + π(π₯) β (πΏ1 + πΏ2 )| = || π (π₯) β πΏ1 + π(π₯) β πΏ2 || | | | | )| |( )| |( β€ | π (π₯) β πΏ1 | + | π(π₯) β πΏ2 | | | | | π π β€ + = π. 2 2 This proves limπ₯βπ (π (π₯) + π(π₯)) = limπ₯βπ π (π₯) + limπ₯βπ π(π₯), which is the result we wanted to prove.
33. (a) We need to show that for any given π > 0, there is a πΏ > 0 so that β |π₯ β π| < πΏ implies |π (π₯)π(π₯)| < π. If π > 0 is given, choose πΏ1 so that when |π₯ β π| < πΏ1 , we have |π (π₯)| < π. This can be done since limπ₯β0 π (π₯) = 0. β Similarly, choose πΏ2 so that when |π₯ β π| < πΏ2 , we have |π(π₯)| < π. Then, if we take πΏ to be the smaller of πΏ1 β β and πΏ2 , weβll have that |π₯ β π| < πΏ implies both |π (π₯)| < π and |π(π₯)| < π. So when |π₯ β π| < πΏ, we have β β |π (π₯)π(π₯)| = |π (π₯)| |π(π₯)| < π β π = π. Thus lim π (π₯)π(π₯) = 0. π₯βπ ( )( ) (b) π (π₯) β πΏ1 π(π₯) β πΏ2 + πΏ1 π(π₯) + πΏ2 π (π₯) β πΏ1 πΏ2 = π((π₯)π(π₯) β πΏ)1 π(π₯) β πΏ2 π (π₯) + πΏ1 πΏ2 + πΏ1 π(π₯) + πΏ2 π (π₯) β πΏ1 πΏ2 = π (π₯)π(π₯). ( ) (c) lim π (π₯) β πΏ1 = lim π (π₯) β lim πΏ1 = πΏ1 β πΏ1 = 0, using the second limit property. Similarly, lim π(π₯) β πΏ2 = 0. π₯βπ π₯βπ π₯βπ π₯βπ ( ) ( ) ( )( ) (d) Since lim π (π₯) β πΏ1 = lim π(π₯) β πΏ2 = 0, we have that lim π (π₯) β πΏ1 π(π₯) β πΏ2 = 0 by part (a). π₯βπ π₯βπ π₯βπ (e) From part (b), we have (( )( ) ) π (π₯) β πΏ1 π(π₯) β πΏ2 + πΏ1 π(π₯) + πΏ2 π (π₯) β πΏ1 πΏ2 ( )( ) = lim π (π₯) β πΏ1 π(π₯) β πΏ2 + lim πΏ1 π(π₯) + lim πΏ2 π (π₯) + lim(βπΏ1 πΏ2 )
lim π (π₯)π(π₯) = lim π₯βπ
π₯βπ π₯βπ
π₯βπ
(using limit property 2) = 0 + πΏ1 lim π(π₯) + πΏ2 lim π (π₯) β πΏ1 πΏ2 π₯βπ
π₯βπ
(using limit property 1 and part (d)) = πΏ1 πΏ2 + πΏ2 πΏ1 β πΏ1 πΏ2 = πΏ1 πΏ2 .
Strengthen Your Understanding 34. False. For example, deο¬ne π as follows: π (π₯) =
{
2π₯ + 1 if π₯ β 2.99 1000 if π₯ = 2.99.
Then π (2.9) = 2(2.9) + 1 = 6.8, whereas π (2.99) = 1000.
π₯βπ
π₯βπ
128
Chapter One /SOLUTIONS
35. False. For example, deο¬ne π as follows: π (π₯) =
{
2π₯ + 1 β1000
if π₯ β 3.01 if π₯ = 3.01.
Then π (3.1) = 2(3.1) + 1 = 7.2, whereas π (3.01) = β1000. 36. False. For some functions we need to pick smaller values of πΏ. For example, if π (π₯) = π₯1β3 + 2 and π = 0 and πΏ = 2, then π (π₯) is within 10β3 of 2 if |π₯1β3 | < 10β3 . This only happens if π₯ is within (10β3 )3 = 10β9 of 0. If π₯ = 10β3 then π₯1β3 = (10β3 )1β3 = 10β1 , which is too large. 37. False. The deο¬nition of a limit guarantees that, for any positive π, there is a πΏ. This statement, which guarantees an π for a speciο¬c πΏ = 10β3 , is not equivalent to limπ₯βπ π (π₯) = πΏ. For example, consider a function with a vertical asymptote within 10β3 of 0, such as π = 0, πΏ = 0, π (π₯) = π₯β(π₯ β 10β4 ). 38. True. This is equivalent to the deο¬nition of a limit. 39. False. Although π₯ may be far from π, the value of π (π₯) could be close to πΏ. For example, suppose π (π₯) = πΏ, the constant function. 40. False. The deο¬nition of the limit says that if π₯ is within πΏ of π, then π (π₯) is within π of πΏ, not the other way round.
Solutions for Chapter 1 Review EXERCISES 1. The line of slope π through the point (π₯0 , π¦0 ) has equation π¦ β π¦0 = π(π₯ β π₯0 ), so the line we want is π¦ β 0 = 2(π₯ β 5) π¦ = 2π₯ β 10. 2. We want a function of the form π¦ = π(π₯ β β)2 + π, with π < 0 because the parabola opens downward. Since (β, π) is the vertex, we must take β = 2, π = 5, but we can take any negative value of π. Figure 1.138 shows the graph with π = β1, namely π¦ = β(π₯ β 2)2 + 5. π¦
(2, 5)
π₯
Figure 1.138: Graph of π¦ = β(π₯ β 2)2 + 5 3. A parabola with π₯-intercepts Β±1 has an equation of the form π¦ = π(π₯ β 1)(π₯ + 1). Substituting the point π₯ = 0, π¦ = 3 gives
3 = π(β1)(1)
so
π = β3.
Thus, the equation we want is π¦ = β3(π₯ β 1)(π₯ + 1) π¦ = β3π₯2 + 3.
SOLUTIONS to Review Problems for Chapter One 4. The equation of the whole circle is
129
β π₯2 + π¦2 = ( 2)2 , β π¦ = β 2 β π₯2 .
so the bottom half is
5. A circle with center (β, π) and radius π has equation (π₯ β β)2 + (π¦ β π)2 = π2 . Thus β = β1, π = 2, and π = 3, giving (π₯ + 1)2 + (π¦ β 2)2 = 9. Solving for π¦, and taking the positive square root gives the top half, so (π¦ β 2)2 = 9 β (π₯ + 1)2 β π¦ = 2 + 9 β (π₯ + 1)2 . See Figure 1.139. π¦
3 -
(β1, 2)
π₯
β Figure 1.139: Graph of π¦ = 2 + 9 β (π₯ + 1)2 6. A cubic polynomial of the form π¦ = π(π₯ β 1)(π₯ β 5)(π₯ β 7) has the correct intercepts for any value of π β 0. Figure 1.140 shows the graph with π = 1, namely π¦ = (π₯ β 1)(π₯ β 5)(π₯ β 7). π¦
1
5
7
π₯
Figure 1.140: Graph of π¦ = (π₯ β 1)(π₯ β 5)(π₯ β 7) 7. Since the vertical asymptote is π₯ = 2, we have π = β2. The fact that the horizontal asymptote is π¦ = β5 gives π = β5. So β5π₯ . π₯β2 8. The amplitude of this function is 5, and its period is 2π, so π¦ = 5 cos π₯. π¦=
9. See Figure 1.141. heart rate
time
administration of drug
Figure 1.141
130
Chapter One /SOLUTIONS
10. Factoring gives
(2 β π₯)(2 + π₯) . π₯(π₯ + 1) The values of π₯ which make π(π₯) undeο¬ned are π₯ = 0 and π₯ = β1, when the denominator is 0. So the domain is all π₯ β 0, β1. Solving π(π₯) = 0 means one of the numeratorβs factors is 0, so π₯ = Β±2. π(π₯) =
11. (a) The domain of π is the set of values of π₯ for which the function is deο¬ned. Since the function is deο¬ned by the graph and the graph goes from π₯ = 0 to π₯ = 7, the domain of π is [0, 7]. (b) The range of π is the set of values of π¦ attainable over the domain. Looking at the graph, we can see that π¦ gets as high as 5 and as low as β2, so the range is [β2, 5]. (c) Only at π₯ = 5 does π (π₯) = 0. So 5 is the only zero of π (π₯). (d) Looking at the graph, we can see that π (π₯) is decreasing on (1, 7). (e) The graph indicates that π (π₯) is concave up at π₯ = 6. (f) The value π (4) is the π¦-value that corresponds to π₯ = 4. From the graph, we can see that π (4) is approximately 1. (g) This function is not invertible, since it fails the horizontal-line test. A horizontal line at π¦ = 3 would cut the graph of π (π₯) in two places, instead of the required one. 12. (a) π (π) + π(π) = (3π2 β 2) + (π + 1) = 3π2 + π β 1. (b) π (π)π(π) = (3π2 β 2)(π + 1) = 3π3 + 3π2 β 2π β 2. (c) The domain of π (π)βπ(π) is deο¬ned everywhere where π(π) β 0, i.e. for all π β β1. (d) π (π(π)) = 3(π + 1)2 β 2 = 3π2 + 6π + 1. (e) π(π (π)) = (3π2 β 2) + 1 = 3π2 β 1. 13. (a) Since π = π (π΄), we see that π (100) represents the value of π when π΄ = 100. Thus π (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 = π (π΄), we have π΄ = π β1 (π). We see that π β1 (75) represents the value of π΄ when π = 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 π‘ log 5 = log 7, so π‘ = log 5 log 2 β 35.003. 15. π‘ = log 1.02 ( )π‘ 16. Collecting similar factors yields 32 = 57 , so ( ) log 57 π‘= ( ) = β0.830. log 32 17. Collecting similar factors yields
(
1.04 1.03
)π‘
= 12.01 . Solving for π‘ yields 5.02 ) ( log 12.01 5.02 π‘= ( ) = 90.283. log 1.04 1.03
18. We want 2π‘ = πππ‘ so 2 = ππ and π = ln 2 = 0.693. Thus π = π0 π0.693π‘ . 19. We want 0.2π‘ = πππ‘ so 0.2 = ππ and π = ln 0.2 = β1.6094. Thus π = 5.23πβ1.6094π‘ . 20. π (π₯) = ln π₯, 3
21. π (π₯) = π₯ ,
π(π₯) = π₯3 . (Another possibility: π (π₯) = 3π₯,
π(π₯) = ln π₯.)
π(π₯) = ln π₯.
22. The amplitude is 5. The period is 6π. See Figure 1.142. π¦ 5
β6π β 9π β3π β 3π 2
2
3π 2
3π
β5
Figure 1.142
9π 2
π₯
( ) 6π π¦ = 5 sin 13 π₯
SOLUTIONS to Review Problems for Chapter One
131
23. The amplitude is 2. The period is 2πβ5. See Figure 1.143. π¦ 6 4 2 β 4π 5
π¦ = 4 β 2 cos(5π₯)
β 2π 5
2π 5
4π 5
π₯
Figure 1.143
24. (a) We determine the amplitude of π¦ by looking at the coeο¬cient of the cosine term. Here, the coeο¬cient is 1, so the amplitude of π¦ is 1. Note that the constant term does not aο¬ect the amplitude. (b) We know that the cosine function cos π₯ repeats itself at π₯ = 2π, so the function cos(3π₯) must repeat itself when 3π₯ = 2π, or at π₯ = 2πβ3. So the period of π¦ is 2πβ3. Here as well the constant term has no eο¬ect. (c) The graph of π¦ is shown in the ο¬gure below. π¦ 6 5 4
2π 3
π₯
25. (a) Since π (π₯) is an odd polynomial with a positive leading coeο¬cient, it follows that π (π₯) β β as π₯ β β and π (π₯) β ββ as π₯ β ββ. (b) Since π (π₯) is an even polynomial with negative leading coeο¬cient, it follows that π (π₯) β ββ as π₯ β Β±β. (c) As π₯ β Β±β, π₯4 β β, so π₯β4 = 1βπ₯4 β 0. (d) As π₯ β Β±β, the lower-degree terms of π (π₯) become insigniο¬cant, and π (π₯) becomes approximated by the highest degree terms in its numerator and denominator. So as π₯ β Β±β, π (π₯) β 6. 26. Exponential growth dominates power growth as π₯ β β, so 10 β 2π₯ is larger. 27. As π₯ β β, 0.25π₯1β2 is larger than 25,000π₯β3 . 28. This is a line with slope β3β7 and π¦-intercept 3, so a possible formula is 3 π¦ = β π₯ + 3. 7 29. Starting with the general exponential equation π¦ = π΄πππ₯ , we ο¬rst ο¬nd that for (0, 1) to be on the graph, we must have π΄ = 1. Then to make (3, 4) lie on the graph, we require 4 = π3π ln 4 = 3π ln 4 β 0.4621. π= 3 Thus the equation is
π¦ = π0.4621π₯ .
Alternatively, we can use the form π¦ = ππ₯ , in which case we ο¬nd π¦ = (1.5874)π₯ .
132
Chapter One /SOLUTIONS
30. This looks like an exponential function. The π¦-intercept is 3 and we use the form π¦ = 3πππ‘ . We substitute the point (5, 9) to solve for π: 9 = 3ππ5 3 = π5π ln 3 = 5π π = 0.2197. A possible formula is
π¦ = 3π0.2197π‘ .
Alternatively, we can use the form π¦ = 3ππ‘ , in which case we ο¬nd π¦ = 3(1.2457)π‘ . 31. π¦ = βππ₯(π₯ + 5) = βπ(π₯2 + 5π₯), where π > 0 is any constant. 32. Since this function has a π¦-intercept at (0, 2), we expect it to have the form π¦ = 2πππ₯ . Again, we ο¬nd π by forcing the other point to lie on the graph: 1 = 2π2π 1 = π2π 2 ( ) 1 = 2π ln 2 ln( 21 ) π= β β0.34657. 2 This value is negative, which makes sense since the graph shows exponential decay. The ο¬nal equation, then, is π¦ = 2πβ0.34657π₯ . Alternatively, we can use the form π¦ = 2ππ₯ , in which case we ο¬nd π¦ = 2(0.707)π₯ . 33. π§ = 1 β cos π 34. π¦ = π(π₯ + 2)(π₯ + 1)(π₯ β 1) = π(π₯3 + 2π₯2 β π₯ β 2), where π > 0 is any constant. 35. π₯ = ππ¦(π¦ β 4) = π(π¦2 β 4π¦), where π > 0 is any constant. ( ) ππ‘ 36. π¦ = 5 sin 20 37. This looks like a fourth degree polynomial with roots at β5 and β1 and a double root at 3. The leading coeο¬cient is negative, and so a possible formula is π¦ = β(π₯ + 5)(π₯ + 1)(π₯ β 3)2 . 38. This looks like a rational function. There are vertical asymptotes at π₯ = β2 and π₯ = 2 and so one possibility for the denominator is π₯2 β 4. There is a horizontal asymptote at π¦ = 3 and so the numerator might be 3π₯2 . In addition, π¦(0) = 0 which is the case with the numerator of 3π₯2 . A possible formula is π¦=
3π₯2 π₯2 β 4
.
39. There are many solutions for a graph like this one. The simplest is π¦ = 1 β πβπ₯ , which gives the graph of π¦ = ππ₯ , ο¬ipped over the π₯-axis and moved up by 1. The resulting graph passes through the origin and approaches π¦ = 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 π (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 π₯ . π (π₯) = sin 5 42. Since the denominator, π₯2 + 1, is continuous and never zero, π(π₯) is continuous on [β1, 1].
SOLUTIONS to Review Problems for Chapter One
133
43. Since
1 1 = , (1 β π₯)(1 + π₯) 1 β π₯2 we see that β(π₯) is not deο¬ned at π₯ = β1 or at π₯ = 1, so β(π₯) is not continuous on [β1, 1]. β(π₯) =
44. (a) lim π (π₯) = 1. π₯β0
(b) lim π (π₯) does not exist. π₯β1
(c) lim π (π₯) = 1. π₯β2
(d) limβ π (π₯) = 0. π₯β3
β§ π₯3 (2π₯ β 6) 3 π₯>3 π₯3 |2π₯ β 6| βͺ π₯ β 3 = 2π₯ , 45. π (π₯) = =β¨ 3 π₯ (β2π₯ + 6) π₯β3 βͺ = β2π₯3 , π₯ < 3 β© π₯β3 Figure 1.144 conο¬rms that lim+ π (π₯) = 54 while limβ π (π₯) = β54; thus lim π (π₯) does not exist. π₯β3
π₯β3
π₯β3
100
π (π₯)
50 0
1
2 3
4
π₯
β50 β100
Figure 1.144 β§ ππ₯ β1 < π₯ < 0 βͺ 46. π (π₯) = β¨ 1 π₯=0 βͺ 0<π₯<1 β© cos π₯ Figure 1.145 conο¬rms that limβ π (π₯) = limβ ππ₯ = π0 = 1, and that lim π (π₯) = lim cos π₯ = cos 0 = 1, so lim π (π₯) = 1.
π₯β0
π₯β0
π₯β0+
π₯β0+
π₯β0
1 π (π₯)
β1
0
1
π₯
Figure 1.145 47. (a) As π‘ approaches β2 from either side, the values of π(π‘) get closer and closer to β5, so the limit appears to be about β5. (b) As π‘ approaches 0 from either side, the values of π(π‘) get closer and closer to β1, so the limit appears to be about β1. (c) As π‘ approaches 1, the values of π(π‘) get closer and closer to 4 on one side of π‘ = 1 and get closer and closer to a value less than 1 on the other side of π‘ = 1. Thus the limit does not exist. (d) As π‘ approaches 3 from either side, the values of π(π‘) become arbitrarily large, so the limit does not exist. 48. (a) As π₯ approaches β2 from either side, the values of π (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 π (π₯) get closer and closer to 7. (Recall that to ο¬nd 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 π (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 π (π₯) get closer and closer to 8. (Again, recall that we donβt 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₯2β3 is deο¬ned for all π₯. 51. No, because sin 0 = 0. 52. No, because ππ₯ β 1 = 0 at π₯ = 0. 53. For β1 β€ π β€ 1, β1 β€ π¦ β€ 1, the graph of π¦ =
cos π β 1 is shown in Figure 1.146. The graph suggests that π cos π β 1 = 0. lim πβ0 π π¦
1 π¦ = cosππβ1
β1
π
1
β1
Figure 1.146 54. For β0.5 β€ π β€ 0.5, 0 β€ π¦ β€ 0.5, the graph of π¦ = curve, we see that lim
π
πβ0 tan(3π)
π is shown in Figure 1.147. Therefore, by tracing along the tan(3π)
= 0.3333 β¦. π¦ 0.5
β0.5
π π¦ = tan(3π)
0
0.5
π
Figure 1.147 3β β 1 in a window such as β0.5 β€ β β€ 0.5 and 0 β€ π¦ β€ 1.5 appears to indicate π¦ β 1.1 as β β 0. By 55. A graph of π¦ = β zooming in on the graph, we can estimate the limit more accurately. Therefore, we estimate that 3β β 1 = 1.098. ββ0 β lim
sin(3β) in a window such as β0.5 β€ β β€ 0.5 and 0 β€ π¦ β€ 4 appears to indicate π¦ β 3 as β β 0. 56. A graph of π¦ = β Therefore, we estimate that sin(3β) = 3. lim ββ0 β 57. (a) Substituting π₯-values into π (π₯) gives: π₯
0.9
0.99
1.01
1.1
π (π₯)
1.054
1.005
0.995
0.953
(b) Since the values of π (π₯) appear to get closer and closer to 1 as π₯ gets closer and closer to 1, we estimate lim
ln π₯
π₯β1 π₯ β 1
Notice that π (π₯) =
ln π₯ is undeο¬ned at π₯ = 1. π₯β1
= 1.
SOLUTIONS to Review Problems for Chapter One
135
58. (a) Substituting π₯-values into π (π₯) gives: π₯
0.9
0.99
1.01
1.1
π (π₯)
1.949
1.995
2.005
2.049
(b) Since the values of π (π₯) appear to get closer and closer to 2 as π₯ gets closer and closer to 1, we estimate π₯β1 = 2. lim β π₯β1 π₯β1 π₯β1 is undeο¬ned at π₯ = 1. Notice that π (π₯) = β π₯β1 59. Since the value of π₯2 increases faster than the value of ln π₯, we know that lim
π₯ββ
ln π₯ approaches zero as π₯ β β. π₯2
ln π₯ = 0. π₯2 60. Since the value of ππ₯ β 2 grows arbitrarily large as π₯ β β while the numerator remains constant, the value of the function approaches zero. 2 = 0. Thus, lim π₯ π₯ββ π β 2 61. For large values of π₯, β5π₯2 + 2 behaves like β5π₯2 and 3π₯2 behaves like 3π₯2 , so (β5π₯2 + 2)β(3π₯2 ) behaves like β5π₯2 β3π₯2 . Thus 5 β5π₯2 + 2 β5π₯2 lim = lim =β . 2 π₯ββ π₯ββ 3π₯2 3 3π₯ Thus, lim
π₯ββ
though answers will vary. 62. Possible answers are π (π₯) = π₯ + 4 and π (π₯) = 5π₯β5 π₯β1 2
63. Possible answers are π (π₯) = 12 + π₯1 and π (π₯) = 2π₯π₯2 +3 though answers will vary. 64. (a) When π₯ < 2, π(π₯) = π₯2 β π₯. So as π₯ approaches 2 from the left, π(π₯) approaches 22 β 2 = 2. So lim π(π₯) = 2.
π₯β2β
(b) When π₯ > 2, π(π₯) = 4βπ₯. So as π₯ approaches 2 from the right, π(π₯) approaches 4β2 = 2. So lim π(π₯) = 2.
π₯β2+
(c) As π₯ approaches 2 from either side, π(π₯) approaches 2. Therefore, lim π(π₯) = 2. π₯β2
(d) For π₯ > 2, π(π₯) = 4βπ₯. As π₯ approaches 3 from the left, π₯ is greater than 2, so π(π₯) approaches 4β3. Thus lim π(π₯) =
π₯β3β
4 . 3
65. (a) For π₯ < 2, we have π (π₯) = 3π₯ β 5, so as π₯ approaches 2 from the left, we have lim π (π₯) = 3(2) β 5 = 1.
π₯β2β
(b) For π₯ > 2, we have π (π₯) = 3 β 2π₯, so as π₯ approaches 2 from the right, we have lim π (π₯) = 3 β 2(2) = β1.
π₯β2+
(c) The one-sided limits limβ π (π₯) and lim+ π (π₯) do not agree. Therefore, the limit lim π (π₯) does not exist, since π (π₯) π₯β2
π₯β2
π₯β2
does not approach a single value as π₯ approaches 2 from both sides. (d) If we are looking at the behavior of π (π₯) close to π₯ = 0, then we are looking at values of π (π₯) for π₯ β€ 2. So for values of π₯ near zero, π (π₯) = 3π₯ β 5. As π₯ approaches zero, π (π₯) approaches 3(0) β 5 = β5. Therefore, lim π (π₯) = β5. π₯β0
136
Chapter One /SOLUTIONS
66. (a) When π₯ < 0, π(π₯) = π₯ + 3. So as π₯ approaches 0 from the left, π(π₯) approaches 0 + 3 = 3. Thus lim π(π₯) = 3.
π₯β0β
(b) When π₯ > 0, π(π₯) = π₯3 + 1. So as π₯ approaches 0 from the right, π(π₯) approaches 03 + 1 = 1. Thus lim π(π₯) = 1.
π₯β0+
(c) The left-hand and right-hand limits of π(π₯) at π₯ = 0 do not agree. Therefore, lim π(π₯) does not exist, since there is no π₯β0
single value that π(π₯) approaches as π₯ approaches 0 from both sides. (d) No matter what the value of π‘ is, π‘2 β₯ 0. So for all π‘, π(π‘2 ) = (π‘2 )3 + 1 = π‘6 + 1. So as π‘ approaches 0 from either side, π(π‘2 ) approaches 06 + 1 = 1. Therefore, lim π(π‘2 ) = 1. π‘β0
67. Evaluating
2
π₯ β 25 at π₯ = 5 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯β5 (π₯ + 5)(π₯ β 5) π₯2 β 25 = . π₯β5 π₯β5
Since π₯ β 5 in the limit, we can cancel the common factor π₯ β 5 to see lim π₯β5
68. Evaluating
(π₯ + 5)(π₯ β 5) π₯2 β 25 = lim = lim(π₯ + 5) = 10. π₯β5 π₯β5 π₯β5 π₯β5
π₯β4 at π₯ = 4 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯2 β 16 π₯β4 π₯β4 = . (π₯ + 4)(π₯ β 4) π₯2 β 16
Since π₯ β 4 in the limit, we can cancel the common factor π₯ β 4 to see lim
π₯β4
π₯β4 π₯2 β 16
69. Evaluating
= lim
π₯β4
π₯β4 (π₯ + 4)(π₯ β 4)
= lim
1
π₯β4 π₯ + 4
=
1 . 8
π₯2 β 5π₯ + 6 at π₯ = 2 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯β2 (π₯ β 3)(π₯ β 2) π₯2 β 5π₯ + 6 = . π₯β2 π₯β2
Since π₯ β 2 in the limit, we can cancel the common factor π₯ β 2 to see lim π₯β2
70. Evaluating
(π₯ β 3)(π₯ β 2) π₯2 β 5π₯ + 6 = lim = lim(π₯ β 3) = β1. π₯β2 π₯β2 π₯β2 π₯β2
π₯β3 at π₯ = 3 gives us 0β0, so we see if we can rewrite the function using algebra. We have π₯2 + 2π₯ β 15 π₯β3 π₯β3 = . (π₯ + 5)(π₯ β 3) π₯2 + 2π₯ β 15
Since π₯ β 3 in the limit, we can cancel the common factor π₯ β 3 to see lim
π₯β3
π₯β3 π₯2 + 2π₯ β 15
= lim
π₯β3
π₯β3 (π₯ + 5)(π₯ β 3)
= lim
1
π₯β3 π₯ + 5
=
1 . 8
β π₯2 + 8π₯ β 2 is continuous everywhere on its domain (that is, at every point except π₯ = Β± 2.) In particular, 2 π₯ β2 it is continuous at π₯ = 2 so we ο¬nd the limit by evaluating the expression at π₯ = 2. We have
71. The expression
18 π₯2 + 8π₯ β 2 = = 9. π₯β2 2 π₯2 β 2
lim
SOLUTIONS to Review Problems for Chapter One
137
72. Evaluating the expression at β = 0, we arrive at 0β0. Rewriting the expression using algebra gives lim
ββ0
(4 + β)2 β 42 (16 + 8β + β2 ) β 16 = lim ββ0 β β 8β + β2 = lim ββ0 β β(8 + β) = lim ββ0 β and since β β 0, canceling the common factor of β, we have = lim(8 + β) ββ0
= 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 = 200. If there is no fertilizer, then the yield is 200 bushels. (c) The horizontal intercept is at π = 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 attainable over the domain 0 β€ π β€ 80. Looking at the graph, we can see that π goes as high as 550 and as low as 0. So the range is 0 β€ π β€ 550. (e) Looking at the graph, we can see that π is decreasing near π = 60. (f) Looking at the graph, we can see that π is concave down everywhere, so it is certainly concave down near π = 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 β 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
β32 = 0.8β¦ C β¦
C = β40β¦ = β¦ F.
75. (a) We have the following functions. (i) Since a change in π of $5 results in a decrease in π of 2, the slope of π = π·(π) is β2β5 items per dollar. So 2 π = π β π. 5
138
Chapter One /SOLUTIONS Now we know that when π = 550 we have π = 100, so 2 β 550 5 100 = π β 220 100 = π β
π = 320. Thus a formula is
2 π = 320 β π. 5
(ii) We can solve π = 320 β 25 π for π in terms of π: 5π = 1600 β 2π 2π = 1600 β 5π 5 π = 800 β π. 2 The slope of this function is β5β2 dollars per item, as we would expect. 5 (b) A graph of π = 800 β π is given in Figure 1.149. 2 π (dollars) 800
550
100
320
π (items)
Figure 1.149 76. See Figure 1.150. π (distance)
π‘ (time)
Figure 1.150 77. (a)
(i) If the atoms are moved farther apart, then π > π so, from the graph, πΉ is negative, indicating an attractive force, which pulls the atoms back together. (ii) If the atoms are moved closer together, then π < π so, from the graph, πΉ is positive, indicating an attractive force, which pushes the atoms apart again. (b) At π = π, the force is zero. The answer to part (a)(i) tells us that if the atoms are pulled apart slightly, so π > π, 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 < π, the force tends to push them back apart. Thus, π = π is a stable equilibrium.
SOLUTIONS to Review Problems for Chapter One
139
78. If the pressure at sea level is π0 , the pressure π at altitude β is given by ) ( 0.4 ββ100 , π = π0 1 β 100 since we want the pressure to be multiplied by a factor of (1 β 0.4β100) = 0.996 for each 100 feet we go up to make it decrease by 0.4% over that interval. At Mexico City β = 7340, so the pressure is π = π0 (0.996)7340β100 β 0.745π0 . So the pressure is reduced from π0 to approximately 0.745π0 , a decrease of 25.5%. 79. Assuming the population of Ukraine is declining exponentially, we have population π (π‘) = 46.01πππ‘ at time π‘ years after 2010. Using the 2014 population, we have 45.43 = 46.01πβπβ 4 ) ( 1 45.43 = 0.00317. π = β ln 4 46.01 We want to ο¬nd the time π‘ at which 44 = 46.01πβ0.00317π‘ ln(44β46.01) π‘=β = 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 inο¬ation rate 30 times to get the desired monthly rate π: (
1+
π 100
)1
) ( 0.67 30 = 1+ = 1.2218. 100
Solving for π, we get π = 22.18, so the inο¬ation rate for April was 22.18%. (b) We compound the daily inο¬ation rate 365 times to get a yearly rate π for 2006: (
1+
π 100
)1
) ( 0.67 365 = 1+ = 11.4426. 100
Solving for π , we get π = 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 β 0.152) units of hydroelectric power were consumed in 2012 if π₯ had been consumed in 2011. Similarly, (π₯(1 β 0.152)(1 β 0.025) units of hydroelectric power were consumed in 2013 if π₯ had been consumed in 2012, and (π₯(1 β 0.152)(1 β 0.025)(1 β 0.036) units of hydroelectric power were consumed in 2014 if π₯ had been consumed in 2013. Since π₯(1 β 0.152)(1 β 0.025)(1 β 0.036) = π₯(0.797) = π₯(1 β 0.203), the percent growth in hydroelectric power consumption was β20.3%, 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 = π (π) =
1 π. 2.2
(b) The inverse function is π = 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 π (π₯) is a parabola that opens upward, we have π (π₯) = ππ₯2 + ππ₯ + π with π > 0. Since π(π₯) is a line with negative slope, π(π₯) = π + ππ₯, with slope π < 0. Therefore π(π (π₯)) = π + π(ππ₯2 + ππ₯ + π) = πππ₯2 + πππ₯ + ππ + π. The coeο¬cient of π₯2 is ππ, which is negative. Thus, the graph is a parabola opening downward. 84. (a) is π(π₯) since it is linear. (b) is π (π₯) since it has decreasing slope; the slope starts out about 1 and then decreases to about 1 . (c) is β(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 = 100ππ(2) , we can solve for the growth rate π using the equation: 2π0 = π0 π2π ln 2 = 2π ln 2 . π= 2 Using the growth rate, we wish to solve for the time π‘ in the formula ln 2
π = 100π 2 π‘ where π = 3,200, so ln 2
3,200 = 100π 2 π‘ π‘ = 10 hours. 86. (a) The π¦-intercept of π (π₯) = π ln(π₯ + 2) is π (0) = π ln 2. Since ln 2 is positive, increasing π increases the π¦-intercept. (b) The π₯-intercept of π (π₯) = π ln(π₯ + 2) is where π (π₯) = 0. Since this occurs where π₯ + 2 = 1, so π₯ = β1, increasing π does not aο¬ect the π₯-intercept. 87. Since the factor by which the prices have increased after time π‘ is given by (1.05)π‘ , the time after which the prices have doubled solves 2 = (1.05)π‘ log 2 = log(1.05π‘ ) = π‘ log(1.05) log 2 β 14.21 years. π‘= log 1.05 88. Using the exponential decay equation π = π0 πβππ‘ , we can solve for the substanceβs decay constant π: (π0 β 0.3π0 ) = π0 πβ20π ln(0.7) π= . β20 Knowing this decay constant, we can solve for the half-life π‘ using the formula 0.5π0 = π0 πln(0.7)π‘β20 20 ln(0.5) π‘= β 38.87 hours. ln(0.7) 89. (a) We know the decay follows the equation
π = π0 πβππ‘ ,
and that 10% of the pollution is removed after 5 hours (meaning that 90% is left). Therefore, 0.90π0 = π0 πβ5π 1 π = β ln(0.90). 5 Thus, after 10 hours: π = π0 πβ10((β0.2) ln 0.90) π = π0 (0.9)2 = 0.81π0 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 π = 0.50π0 : 0.50π0 = π0 ππ‘((0.2) ln 0.90) 0.2π‘ )
0.50 = πln(0.90
0.50 = 0.900.2π‘ 5 ln(0.50) π‘= β 32.9 hours. ln(0.90) π
(c) π0
5 10
π‘
32.9
(d) When highly polluted air is ο¬ltered, there is more pollutant per liter of air to remove. If a ο¬xed 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; 0.5π0 = π0 πβ29π ln(1β2) π= . β29 Knowing this, we can look for the time π‘ in which π = 0.10π0 , or 0.10π0 = π0 πln(0.5)π‘β29 29 ln(0.10) π‘= = 96.336 years. ln(0.5) 91. One hour. 92. (a) π0 represents the maximum voltage. (b) The period is 2πβ(120π) = 1β60 second. (c) Since each oscillation takes 1β60 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 1β60 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 1β50 seconds, so it oscillates at 50 cycles per second. 94. (a) The amplitude of the sine curve is |π΄|. Thus, increasing |π΄| stretches the curve vertically. See Figure 1.151. (b) The period of the wave is 2πβ|π΅|. Thus, increasing |π΅| makes the curve oscillate more rapidlyβin other words, the function executes one complete oscillation in a smaller interval. See Figure 1.152.
π΄=3 π΄=2 π΄=1
-
R
3 2 1
β2π
π΅=1
π΅=2
π¦
2π
π¦ 1
?
2π
π₯ β2π
β3
Figure 1.151
π΅=3
β1
Figure 1.152
π₯
142
Chapter One /SOLUTIONS
95. (a)
(i) The water that has ο¬owed out of the pipe in 1 second is a cylinder of radius π and length 3 cm. Its volume is π = ππ2 (3) = 3ππ2 . (ii) If the rate of ο¬ow is π cm/sec instead of 3 cm/sec, the volume is given by π = ππ2 (π) = ππ2 π. (i) The graph of π as a function of π is a quadratic. See Figure 1.153.
(b)
π
π
π
π
Figure 1.153
Figure 1.154
(ii) The graph of π as a function of π is a line. See Figure 1.154. 96. Looking at π, we see that the ratio of the values is: 3.74 4.49 5.39 6.47 3.12 β β β β β 0.83. 3.74 4.49 5.39 6.47 7.76 Thus π is an exponential function, and so π and π are the power functions. Each is of the form ππ₯2 or ππ₯3 , and since π(1.0) = 9.01 we see that for π, the constant coeο¬cient is 9.01. Trial and error gives π(π₯) = 9.01π₯2 , since π(2.2) = 43.61 β 9.01(4.84) = 9.01(2.2)2 . Thus π (π₯) = ππ₯3 and we ο¬nd π by noting that π (9) = 7.29 = π(93 ) so π=
7.29 = 0.01 93
and π (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 at π₯ = 1, π at π₯ = 2, and π at π₯ = 3 and then returning to the π₯-axis at π₯ = 4. See Figure 1.156. π¦
π¦ π
4 3
β1
2
π
1
π 0
1
2
3
4
5
π₯
β1
0
Figure 1.155
1
2
3
4
5
π₯
Figure 1.156
98. (a) Reading the graph of π against π‘ shows that π β 5.2 when π‘ = 1.5. Since the coordinates of π are π₯ = 5 cos π, π¦ = 5 sin π, when π‘ = 1.5 the coordinates are (π₯, π¦) β (5 cos 5.2, 5 sin 5.2) = (2.3, β4.4). (b) As π‘ increases from 0 to 5, the angle π increases from 0 to about 6.3 and then decreases to 0 again. Since 6.3 β 2π, this means that π starts on the π₯-axis at the point (5, 0), moves counterclockwise the whole way around the circle (at which time π β 2π), 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 π¦(π₯) = sin π₯ and π§π (π₯) = ππβπ₯ for π = 1, 2, 4, 6, 8, 10 are shown in Figure 1.157. The values of π (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 ο¬nder on a calculator or computer. From Figure 1.157 it is clear that the smallest solution of sin π₯ = ππβπ₯ for π = 1, 2, 4, 6 occurs on the ο¬rst 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 and 2π, but ππβπ₯ is uniformly positive. Somewhere in the interval 6 β€ π β€ 8, π (π) has a discontinuity.
2
π§π (π₯) = ππβπ₯
+
1 0
6 2
4
Table 1.19
π¦(π₯) = sin π₯
10
12
8
π₯
β1
Figure 1.157
π
π (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 β 10π₯2 = 5π₯2 (π₯ β 2), we can cancel (π₯ β 2) provided π₯ β 2, giving π (π₯) =
5π₯3 β 10π₯2 = 5π₯2 π₯β2
π₯ β 2.
Thus, if we pick π = 5(2)2 = 20, the function is continuous. 102. At π₯ = 0, the curve π¦ = π cos π₯ has π¦ = π cos 0 = π. At π₯ = 0, the curve π¦ = ππ₯ β π has π¦ = π0 β π = 1 β π. If π(π₯) is continuous, we need 1 π = 1 β 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 π‘ β β, 3 β 2πβπ‘ β 3. We shall use limit properties to conο¬rm this. We now calculate the limit in stages using the properties to justify each step: lim (3 β 2πβπ‘ ) = lim (3) + lim (β2πβπ‘ )
(Property 2)
= lim (3) β 2 lim (πβπ‘ )
(Property 1)
π‘ββ
π‘ββ π‘ββ
π‘ββ
π‘ββ
= 3 β 2(0) = 3
(Property 6 and because πβπ‘ β 0)