Understanding nrt reading 1 1 of 2 radiogaphic testing a

Understandings NRT - Reading 1 Radiographic Testing 2nd Pre-exam self study note for Neutron Radiographic Testing 2nd April 2016

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NDT for Upstream

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Charlie Chong/ Fion Zhang

Fion Zhang at Xitang 1st April 2016

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SME- Subject Matter Expert

我们的大学,其实应该聘请这些能干的退休教授. 或许在职的砖头怕被排斥. http://cn.bing.com/videos/search?q=Walter+Lewin&FORM=HDRSC3 https://www.youtube.com/channel/UCiEHVhv0SBMpP75JbzJShqw

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NR - Neutron Radiographic Testing Length: 4 hours Questions: 135 1. Principles/ Theory • Nature of penetrating radiation • Interaction between penetrating radiation and matter • Neutron radiography imaging • Radiometry 2. Equipment/Materials • Sources of neutrons • Radiation detectors • Nonimaging devices

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3. Techniques/Calibrations • Blocking and filtering • Multifilm technique • Enlargement and projection • Stereoradiography • Triangulation methods • Autoradiography • Flash Radiography • In-motion radiography • Fluoroscopy • Electron emission radiography • Microradiography • Laminography (tomography) • Control of diffraction effects • Panoramic exposures • Gaging • Real time imaging • Image analysis techniques

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4. Interpretation/Evaluation • Image-object relationships • Material considerations • Codes, standards, and specifications 5. Procedures • Imaging considerations • Film processing • Viewing of radiographs • Judging radiographic quality 6. Safety and Health • Exposure hazards • Methods of controlling radiation exposure • Operation and emergency procedures

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http://www.yumpu.com/zh/browse/user/charliechong http://issuu.com/charlieccchong

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http://greekhouseoffonts.com/

The Magical Book of Tank Inspection ICP

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数字签名者：菲 菲 DN：cn=菲菲, o= 学无止境, ou=Technical, email=fion_zhang @qq.com, c=CN 日期：2016.04.10 09:27:21 +08'00'

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闭门练功

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Industrial Radiography

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Khanacademy

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https://www.khanacademy.org/science/chemistry/nuclear-chemistry/radioactive-decay/v/types-of-decay

Chapter 1: History of Radiography X-rays were discovered in 1895 by Wilhelm Conrad Roentgen (1845-1923) who was a Professor at Wuerzburg University in Germany.

Working with a cathode-ray tube in his laboratory, Roentgen observed a fluorescent glow of crystals on a table near his tube. The tube that Roentgen was working with consisted of a glass envelope (bulb) with positive and negative electrodes encapsulated in it. The air in the tube was evacuated, and when a high voltage was applied, the tube produced a fluorescent glow. Roentgen shielded the tube with heavy black paper, and discovered a green colored fluorescent light generated by a material located a few feet away from the tube.

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He concluded that a new type of ray was being emitted from the tube. This ray was capable of passing through the heavy paper covering and exciting the phosphorescent materials in the room. He found the new ray could pass through most substances casting shadows of solid objects. Roentgen also discovered that the ray could pass through the tissue of humans, but not bones and metal objects. One of Roentgen's first experiments late in 1895 was a film of the hand of his wife, Bertha. It is interesting that the first use of X-rays were for an industrial (not medical) application as Roentgen produced a radiograph of a set of weights in a box to show his colleagues.

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Wuerzburg University

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Roentgen's discovery was a scientific bombshell, and was received with extraordinary interest by both scientist and laymen. Scientists everywhere could duplicate his experiment because the cathode tube was very well known during this period. Many scientists dropped other lines of research to pursue the mysterious rays.

Newspapers and magazines of the day provided the public with numerous stories, some true, others fanciful, about the properties of the newly discovered rays.

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Taking an X-ray image with early Crookes tube apparatus, late 1800s. The Crookes tube is visible in center. The standing man is viewing his hand with a fluoroscope screen. No precautions against radiation exposure are taken; its hazards were not known at the time.

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Public fancy was caught by this invisible ray with the ability to pass through solid matter, and, in conjunction with a photographic plate, provide a picture of bones and interior body parts. Scientific fancy was captured by demonstration of a wavelength shorter than light. This generated new possibilities in physics, and for investigating the structure of matter. Much enthusiasm was generated about potential applications of rays as an aid in medicine and surgery. Within a month after the announcement of the discovery, several medical radiographs had been made in Europe and the United States which were used by surgeons to guide them in their work. In June 1896, only 6 months after Roentgen announced his discovery, X-rays were being used by battlefield physicians to locate bullets in wounded soldiers.

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Battlefield

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http://www.iimeffwd.marines.mil/Photos.aspx?igphoto=2000023630

Battlefield

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http://www.iimeffwd.marines.mil/Photos.aspx?igphoto=2000023630

Battlefield

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http://www.iimeffwd.marines.mil/Photos.aspx?igphoto=2000023630

Prior to 1912, X-rays were used little outside the realms of medicine, and dentistry, though some X-ray pictures of metals were produced. The reason that X-rays were not used in industrial application before this date was because the X-ray tubes (the source of the X-rays) broke down under the voltages required to produce rays of satisfactory penetrating power for industrial purpose. However, that changed in 1913 when the high vacuum Xray tubes designed by Coolidge became available. The high vacuum tubes were an intense and reliable X-ray sources, operating at energies up to 100,000 volts. (0.1Mv) In 1922, industrial radiography took another step forward with the advent of the 200,000-volt X-ray tube that allowed radiographs of thick steel parts to be produced in a reasonable amount of time. In 1931, General Electric Company developed 1,000,000 volt X-ray generators, providing an effective tool for industrial radiography. That same year, the American Society of Mechanical Engineers (ASME) permitted X-ray approval of fusion welded pressure vessels that further opened the door to industrial acceptance and use.

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A Second Source of Radiation Shortly after the discovery of X-rays, another form of penetrating rays was discovered. In 1896, French scientist Henri Becquerel discovered natural radioactivity. Many scientists of the period were working with cathode rays, and other scientists were gathering evidence on the theory that the atom could be subdivided. Some of the new research showed that certain types of atoms disintegrate by themselves. It was Henri Becquerel who discovered this phenomenon while investigating the properties of fluorescent minerals.

Becquerel was researching the principles of fluorescence, certain minerals glow (fluoresce) when exposed to sunlight. He utilized photographic plates to record this fluorescence.

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One of the minerals Becquerel worked with was a uranium compound. On a day when it was too cloudy to expose his samples to direct sunlight, Becquerel stored some of the compound in a drawer with his photographic plates. Later when he developed these plates, he discovered that they were fogged (exhibited exposure to light.) Becquerel questioned what would have caused this fogging? He knew he had wrapped the plates tightly before using them, so the fogging was not due to stray light. In addition, he noticed that only the plates that were in the drawer with the uranium compound were fogged. Becquerel concluded that the uranium compound gave off a type of radiation that could penetrate heavy paper and expose photographic film.

Becquerel continued to test samples of uranium compounds and determined that the source of radiation was the element uranium. Bacquerel's discovery was, unlike that of the X-rays, virtually unnoticed by laymen and scientists alike. Only a relatively few scientists were interested in Becquerel's findings. It was not until the discovery of radium by the Curies two years later that interest in radioactivity became wide spread.

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Becquerel

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While working in France at the time of Becquerel's discovery, Polish scientist Marie Curie became very interested in his work. She suspected that a uranium ore known as pitchblende contained other radioactive elements.

Marie and her husband, a French scientist, Pierre Curie started looking for these other elements. In 1898, the Curies discovered another radioactive element in pitchblende, they named it 'polonium' in honor of Marie Curie's native homeland. Later that year, the Curie's discovered another radioactive element which they named 'radium', or shining element. Both polonium and radium were more radioactive than uranium. Since these discoveries, many other radioactive elements have been discovered or produced.

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Radium became the initial industrial gamma ray source. The material allowed radiographing castings up to 10 to 12 inches thick. During World War II, industrial radiography grew tremendously as part of the Navy's shipbuilding program. In 1946, manmade gamma ray sources such as cobalt and iridium became available. These new sources were far stronger than radium and were much less expensive. The manmade sources rapidly replaced radium, and use of gamma rays grew quickly in industrial radiography.

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Health Concerns The science of radiation protection, or "health physics" as it is more properly called, grew out of the parallel discoveries of X-rays and radioactivity in the closing years of the 19th century. Experimenters, physicians, laymen, and physicists alike set up X-ray generating apparatus and proceeded about their labors with a lack of concern regarding potential dangers. Such a lack of concern is quite understandable, for there was nothing in previous experience to suggest that X-rays would in any way be hazardous. Indeed, the opposite was the case, for who would suspect that a ray similar to light but unseen, unfelt, or otherwise undetectable by the senses would be damaging to a person? More likely, or so it seemed to some, X-rays could be beneficial for the body.

Inevitably, the widespread and unrestrained use of X-rays led to serious injuries. Often injuries were not attributed to X-ray exposure, in part because of the slow onset of symptoms, and because there was simply no reason to suspect X-rays as the cause. Some early experimenters did tie X-ray exposure and skin burns together. The first warning of possible adverse effects of X-rays came from Thomas Edison, William J. Morton, and Nikila Tesla who each reported eye irritations from experimentation with X-rays and fluorescent substances.

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Today, it can be said that radiation ranks among the most thoroughly investigated causes of disease. Although much still remains to be learned, more is known about the mechanisms of radiation damage on the molecular, cellular, and organ system than is known for most other health stressing agents. Indeed, it is precisely this vast accumulation of quantitative doseresponse data that enables health physicists to specify radiation levels so that medical, scientific, and industrial uses of radiation may continue at levels of risk no greater than, and frequently less than, the levels of risk associated with any other technology.

X-rays and Gamma rays are electromagnetic radiation of exactly the same nature as light, but of much shorter wavelength. Wavelength of visible light is of the order of 6000 angstroms while the wavelength of x-rays is in the range of one angstrom and that of gamma rays is 0.0001 angstrom. This very short wavelength is what gives x-rays and gamma rays their power to penetrate materials that light cannot.

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These electromagnetic waves are of a high energy level and can break chemical bonds in materials they penetrate. If the irradiated matter is living tissue the breaking of chemical bond may result in altered structure or a change in the function of cells.

Early exposures to radiation resulted in the loss of limbs and even lives. Men and women researchers collected and documented information on the interaction of radiation and the human body. This early information helped science understand how electromagnetic radiation interacts with living tissue.

Unfortunately, much of this information was collected at great personal expense.

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Health Concerns

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http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Health Concerns

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http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Charlie Chong/ Fion Zhang

Health Concerns

http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Health Concerns

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http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Health Concerns

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http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Health Concerns

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http://v.youku.com/v_show/id_XMTY1MzAwMTQw.html

Present State of Radiography In many ways radiography has changed little from the early days of its use.

We still capture a shadow image on film using similar procedures and processes technicians were using in the late 1800's. Today, however, we are able to generate images of higher quality, and greater sensitivity through the use of higher quality films with a larger variety of film grain sizes. Film processing has evolved to an automated state producing more consistent film quality by removing manual processing variables. Electronics and computers allow technicians to now capture images digitally. The use of "filmless radiography" provides a means of capturing an image, digitally enhancing, sending the image anywhere in the world, and archiving an image that will not deteriorate with time. Technological advances have provided industry with smaller, lighter, and very portable equipment that produce high quality X-rays.

The use of linear accelerator provide a means of generating extremely short wavelength, highly penetrating radiation, a concept dreamed of only a few short years ago. While the process has changed little, technology has evolved allowing radiography to be widely used in numerous areas of inspection.

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Filmless Radiography

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http://www.ari.com.au/digital-radiography.html

Filmless Radiography

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http://www.ari.com.au/digital-radiography.html

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http://www.ari.com.au/digital-radiography.html

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http://www.ari.com.au/digital-radiography.html

Radiography has seen expanded usage in industry to inspect not only welds and castings, but to radiographically inspect items such as airbags and caned food products. Radiography has found use in metallurgical material identification and security systems at airports and other facilities.

Gamma ray inspection has also changed considerably since the Curies' discovery of radium. Man-made isotopes of today are far stronger and offer the technician a wide range of energy levels and half-lives. The technician can select Co-60 which will effectively penetrate very thick materials, or select a lower energy isotope, such as Thulium, Tm-170, which can be used to inspect plastics and very thin or low density materials. Today gamma rays find wide application in industries such as petrochemical, casting, welding, and aerospace.

Keywords: Linac Filmless radiography Film grain sizes

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https://en.wikipedia.org/wiki/Isotopes_of_thulium

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https://en.wikipedia.org/wiki/Isotopes_of_thulium

Nature of Penetrating Radiation X-rays and gamma rays are part of the electromagnetic spectrum. They are waveforms as are light rays, microwaves, and radio wave, but x-rays and gamma rays cannot been seen, felt, or heard. They possess no charge and no mass and, therefore, are not influenced by electrical and magnetic fields and will always travel in straight lines. They can be characterized by frequency, wavelength, and velocity. However, they act somewhat like a particle at times in that they occur as small "packets" of energy and are referred to as "photon."

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X-rays and gamma rays differ only in their source of origin. X-rays are produced by an x-ray generator, which will be discussed a little latter. Gamma radiation, which will be the focus of discussion here, is the product of radioactive atoms. Depending upon the ratio of neutrons to protons within its nucleus, an isotope of a particular element may be stable or unstable. Over time the nuclei of unstable isotopes spontaneously disintegrate, or transform, in a process known as radioactive decay. Various types of ionizing radiation may be emitted from the nucleus and/or its surrounding electrons. Nuclides which undergo radioactive decay are called radionuclides. Any material which contains measurable amounts of one or more radionuclides is a radioactive material.

The degree of radioactivity or radiation producing potential of a given amount of radioactive material is measured in Curies (Ci). The curie which was originally defined as that amount of any radioactive material which disintegrates at the same rate as one gram of pure radium. The curie has since been defined more precisely as a quantity of radioactive material in which 3.7 x 1010 atoms disintegrate per second. The International System (SI) unit for activity is the Becquerel (Bq), which is that quantity of radioactive material in which one atom is transformed per second.

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Keywords: The curie - 3.7 x 1010 atoms disintegrate per second.

The Becquerel (Bq) - one atom is transformed per second.

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Beta Decay During beat decay, the parent nuclei emitted beta rays which made up of a beta particle. Beta particle is a fast moving electron or positron which depends on the type on beta decay involved.

1 1 0n → → 1p Charlie Chong/ Fion Zhang

+ -1e1 + Ï…

http://chemistry.tutorvista.com/nuclear-chemistry/alpha-decay.html

Alpha Decay Definition toms with more number of neutrons and protons are highly unstable and get stabilized by emission alpha particles. The emission of alpha particles from parent nuclei to form new daughter nuclei is called as alpha decay.

b aX → → a-2

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Yb-4 +2He4

The radioactivity of a given amount of radioactive material does not depend upon the mass of material present. For example, two one-curie sources of Cs-137 might have very different masses depending upon the relative proportion of non-radioactive atoms present in each source. Radioactivity is expressed as the number of curies or becquerels per unit mass or volume.

Each radionuclide decays at its own unique rate which cannot be altered by any chemical or physical process.

A useful measure of this rate is the half-life of the radionuclide. Half-life is defined as the time required for the activity of any particular radionuclide to decrease to one-half of its initial value, or one-half of the atoms to change to daughter atoms reverting to a stable state material. Half-lives of radionuclides range from microseconds to billions of years. Half-life of two widely used industrial isotopes are 75 days for Iridium-192, and 5.3 years for Cobalt-60.

More exacting calculations can be made for the half-life of these materials, however, these times are commonly used by technicians.

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Keywords: Half-life of two widely used industrial isotopes are for: T½ Iridium-192- 75 days T½ Cobalt-60- 5.3 years

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https://en.wikipedia.org/wiki/Cobalt-60

Cobalt-60, 60Co, is a synthetic radioactive isotope of cobalt with a half-life of 5.2714 years. It is produced artificially in nuclear reactors. Deliberate industrial production depends on neutron activation of bulk samples of the monoisotopic and mononuclidic cobalt isotope 59Co.Measurable quantities are also produced as a by-product of typical nuclear power plant operation and may be detected externally when leaks occur. In the latter case (in the absence of added cobalt) the incidentally produced 60Co is largely the result of multiple stages of neutron activation of iron isotopes in the reactor's steel structures via the creation of 5960Co precursor. The simplest case of the latter would result from the activation of 5826Fe. 6027Co decays by beta decay to the stable isotope nickel-60 (60Ni). The activated nickel nucleus emits two gamma rays with energies of 1.17 and 1.33 MeV, hence the overall nuclear equation of the reaction is 59

27Co

+ n → 6027Co → 6028Ni + e− + νe + gamma rays

58

26Fe

+ n → 5926Fe → 5927Co + e− + νe + gamma rays

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Half Life Equation:

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Types Ionizing Radiation When an atom undergoes radioactive decay, it emits one or more forms of ionizing radiation, defined as radiation with sufficient energy to ionize the atoms with which it interacts. Ionizing radiation can consist of high speed subatomic particles ejected from the nucleus or electromagnetic radiation (gamma-rays) emitted by either the nucleus or orbital electrons.

Alpha Particles Îą2+, He2+ Certain radionuclides of high atomic mass (Ra226, U238, Pu239) decay by the emission of alpha particles. These alpha particles are tightly bound units of two neutrons and two protons each (42He2+ nucleus) and have a positive charge. Emission of an alpha particle from the nucleus results in a decrease of two units of atomic number (Z) and four units of mass number (A). Alpha particles are emitted with discrete energies characteristic of the particular transformation from which they originate. All alpha particles from a particular radionuclide transformation will have identical energies.

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Alpha Particle

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https://en.wikipedia.org/wiki/Alpha_particle

Alpha particles consist of two protons and two neutrons bound together into a particle identical to a helium nucleus. They are generally produced in the process of alpha decay, but may also be produced in other ways. Alpha particles are named after the first letter in the Greek alphabet, α. The symbol for the alpha particle is α or α2+ . Because they are identical to helium nuclei, they are also sometimes written as He2+ or 42He2+ indicating a helium ion with a +2 charge (missing its two electrons- why do these electron go? Kinetic energy? ). If the ion gains electrons from its environment, the alpha particle can be written as a normal (electrically neutral) helium atom 4 2He (g) .

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Alpha particles, like helium nuclei, have a net spin of zero. Due to the mechanism of their production in standard alpha radioactive decay, alpha particles generally have a kinetic energy of about 5 MeV, and a velocity in the vicinity of 5% the speed of light. (See discussion below for the limits of these figures in alpha decay.) They are a highly ionizing form of particle radiation, and (when resulting from radioactive alpha decay) have low penetration depth.

They are able to be stopped by a few centimeters of air, or by the skin.

However, so-called long range alpha particles from ternary fission are three times as energetic, and penetrate three times as far. As noted, the helium nuclei that form 10–12% of cosmic rays are also usually of much higher energy than those produced by nuclear decay processes, and are thus capable of being highly penetrating and able to traverse the human body and also many meters of dense solid shielding, depending on their energy. To a lesser extent, this is also true of very high-energy helium nuclei produced by particle accelerators.

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When alpha particle emitting isotopes are ingested, they are far more dangerous than their half-life or decay rate would suggest, due to the high relative biological effectiveness of alpha radiation to cause biological damage, after alpha-emitting radioisotopes enter living cells. Ingested alpha emitter radioisotopes (such as transuranics or actinides) are an average of about 20 times more dangerous, and in some experiments up to 1000 times more dangerous, than an equivalent activity of beta emitting or gamma emitting radioisotopes.

In computer technology, dynamic random access memory (DRAM) "soft errors" were linked to alpha particles in 1978 in Intel's DRAM chips. The discovery led to strict control of radioactive elements in the packaging of semiconductor materials, and the problem is largely considered to be solved.

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Anti-alpha particle In 2011, members of the international STAR collaboration using the Relativistic Heavy Ion Collider at the U.S. Department of Energy's Brookhaven National Laboratory detected the antimatter partner of the helium nucleus, also known as the anti-alpha.[13] The experiment used gold ions moving at nearly the speed of light and colliding head on to produce the antiparticle

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http://web2.uwindsor.ca/courses/physics/high_schools/2013/Antimatter/history.html

Anti-alpha particle

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http://www.nbcnews.com/science/space/stephen-hawking-gets-star-treatment-theory-everything-n238441

A Brief History of Antimatter Antimatter has been a topic of great interest for physics enthusiasts for the past 100 years.

As a relatively new topic there have been many recent advances in the theory and technology that has allowed us to observe this phenomenon. The timeline below outlines some of key people and ideas behind our recent understanding of antimatter.

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Beta Particles A nucleus with an unstable ratio of neutrons to protons may decay through the emission of a high speed electron called a beta particle. This results in a net change of one unit of atomic number (Z). Beta particles have a negative charge and the beta particles emitted by a specific radionuclide will range in energy from near zero up to a maximum value, which is characteristic of the particular transformation. (A number remains the same) Gamma-rays A nucleus which is in an excited state may emit one or more photons (packets of electromagnetic radiation) of discrete 分立的 energies. The emission of gamma rays does not alter the number of protons or neutrons in the nucleus but instead has the effect of moving the nucleus from a higher to a lower energy state (unstable to stable). Gamma ray emission frequently follows beta decay, alpha decay, and other nuclear decay processes.

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X-rays are also part of the electromagnetic spectrum and are distinguished from gamma rays only by their source (orbital electrons rather than the nucleus). X-rays are emitted with discrete energies by electrons as they shift orbits following certain types of nuclear decay processes. Internal conversion occurs in a isotope when the energy is transferred to an atomic origin electron that is then ejected with kinetic energy equal to the expected gamma ray, but minus the electron's binding energy. The vacancy in the atomic structure is filled by an external electron, resulting in the production of x-rays. Thulium170 is a good example of this type of disintegration. When Thulium-170 looses its energy it will exhibit a 60 % probability of interaction with an orbital electron thus producing x-radiation.

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Characteristic X-rays are emitted when outer-shell electrons fill a vacancy in the inner shell of an atom, releasing X-rays in a pattern that is "characteristic" to each element. Characteristic X-rays were discovered by Charles Glover Barkla in 1909, who later won the Nobel Prize in Physics for his discovery in 1917.

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https://en.wikipedia.org/wiki/Characteristic_X-ray

Characteristic X-rays are produced when an element is bombarded with highenergy particles, which can be photons, electrons or ions (such as protons).

When the incident particle strikes a bound electron (the target electron) in an atom, the target electron is ejected from the inner shell of the atom. After the electron has been ejected, the atom is left with a vacant energy level, also known as a core hole. Outer-shell electrons then fall into the inner shell, emitting quantized photons with an energy level equivalent to the energy difference between the higher and lower states. Each element has a unique set of energy levels, and thus the transition from higher to lower energy levels produces X-rays with frequencies that are characteristic to each element.

When an electron falls from the L shell to the K shell, the X-ray emitted is called a K-alpha X-ray. Similarly, when an electron falls from the M shell to the K shell, the X-ray emitted is called a K-beta X-ray.[3] Sometimes, however, instead of releasing the energy in the form of an X-ray, the energy can be transferred to another electron, which is then ejected from the atom. This is known as the Auger effect, and the second ejected electron is known as an Auger electron.

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https://en.wikipedia.org/wiki/Characteristic_X-ray

In an X-ray tube, electrons are accelerated in a vacuum by an electric field and shot into a piece of metal called the "target". X-rays are emitted as the electrons slow down (decelerate) in the metal. The output spectrum consists of a continuous spectrum of X-rays, with additional sharp peaks at certain energies (see graph on right). The continuous spectrum is due to bremsstrahlung, while the sharp peaks are characteristic X-rays associated with the atoms in the target. For this reason, bremsstrahlung in this context is also called continuous X-rays.

The spectrum has a sharp cutoff at low wavelength, which is due to the limited energy of the incoming electrons. For example, if an electron in the tube is accelerated through 60 kV, then it will acquire a kinetic energy of 60 keV, and when it strikes the target it can create X-rays with energy of at most 60 keV, by conservation of energy. (This upper limit corresponds to the electron coming to a stop by emitting just one X-ray photon. Usually the electron emits many photons, and each has an energy less than 60 keV.) A photon with energy of at most 60 keV has wavelength of at least 21 pm, so the continuous X-ray spectrum has exactly that cutoff, as seen in the graph.

More generally the formula for the low-wavelength cutoff is

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Spectrum of the X-rays emitted by an X-ray tube with a rhodium target, operated at 60 kV. The continuous curve is due to bremsstrahlung, and the spikes are characteristic K lines for rhodium. The curve goes to zero at 21 pm in agreement with the Duane–Hunt law, as described in the text.

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Characteristic & Bremsstrahlung Radiations

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Bremsstrahlung, from bremsen "to brake" and Strahlung "radiation", i.e. "braking radiation" or "deceleration radiation") is electromagnetic radiation produced by the deceleration of a charged particle when deflected by another charged particle, typically an electron by an atomic nucleus. The moving particle loses kinetic energy, which is converted into a photon, thus satisfying the law of conservation of energy. The term is also used to refer to the process of producing the radiation. Bremsstrahlung has a continuous spectrum, which becomes more intense and whose peak intensity shifts toward higher frequencies as the change of the energy of the accelerated particles increases.

Broadly speaking, Bremsstrahlung or "braking radiation" is any radiation produced due to the deceleration (negative acceleration) of a charged particle, which includes synchrotron radiation, cyclotron radiation, and the emission of electrons and positrons during beta decay. However, the term is frequently used in the more narrow sense of radiation from electrons (from whatever source) slowing in matter.

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Elastic scattering Elastic scattering is a form of particle scattering in scattering theory, nuclear physics and particle physics. In this process, the kinetic energy of a particle is conserved in the center-of-mass frame, but its direction of propagation is modified (by interaction with other particles and/or potentials).

Furthermore, while the particle's kinetic energy in the center-of-mass frame is constant, its energy in the lab frame is not. Generally, elastic scattering describes a process where the total kinetic energy of the system is conserved.

During elastic scattering of high-energy subatomic particles, linear energy transfer (LET) takes place until the incident particle's energy and speed has been reduced to the same as its surroundings, at which point the particle is "stopped."

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Electron elastic scattering When an alpha particle is an incident particle and it is diffracted in the Coulomb potential of atoms and molecules, the elastic scattering process is called Rutherford scattering. In many electron diffraction techniques like reflection high energy electron diffraction (RHEED), transmission electron diffraction (TED), and gas electron diffraction (GED), where the incident electrons have sufficiently high energy (>10 keV), the elastic electron scattering becomes the main component of the scattering process and the scattering intensity is expressed as a function of the momentum transfer defined as the difference between the momentum vector of the incident electron and that of the scattered electron.

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Pictorial description of how an electron beam may interact with a sample with nucleus N, and electron cloud of electron shells K,L,M. Showing transmitted electrons and elastic/inelastic-ally scattered electrons.

SE is a Secondary Electron ejected by the beam electron, emitting a characteristic photon (X-Ray) Îł. BSE is a Back-Scattered Electron, an electron which is scattered backwards instead of being transmitted through the sample.

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Bremsstrahlung, from bremsen "to brake" and Strahlung "radiation", i.e. "braking radiation" or "deceleration radiation") is electromagnetic radiation produced by the deceleration of a charged particle when deflected by another charged particle, typically an electron by an atomic nucleus.

Inelastic or elastic scattering

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■ Neutrons are typically produced by one of three methods. Large amounts of neutrons are produced in nuclear reactors due to the nuclear fission process.

■ High energy neutrons are also produced by accelerating deuterons that causes them to interact with tritium nuclei.

D + T → n + 4He En = 14.1 MeV D + D → n + 3He En = 2.5 MeV

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Nuclear physicist at the Idaho National Laboratory sets up an experiment using an electronic neutron generator.

Charlie Chong/ Fion Zhang

https://en.wikipedia.org/wiki/Neutron_generator

■The third method of producing neutrons is by bombarding beryllium with alpha particles. Neutron sources can be made using the alpha-neutron reaction on beryllium by making a mixture of powered alpha emitter and beryllium and sealing it in a metal container. Early neutron sources used radium as the alpha emitter. Modern neutron sources typically use plutonium or americium as the alpha source. The radium-beryllium (Ra/Be) sources were also sources of large amounts of gamma radiation while the plutoniumberyllium (Pu/Be) sources and the americium-beryllium (Am/Be) sources only produce small amounts of very low energy gamma radiation. Thus, as neutron sources, Pu/Be and Am/Be sources tend to be less hazardous to handle. The older Ra/Be sources also had a tendency to develop leaks over time and give off radon gas, one of the products of radium decay. 注: Ra/Be - Ra as 42He2+ source, Be as alpha target

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron5_1.htm

4

2He

2+

+ 94Be → 126C + n

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/5_neutron.swf

4

2He

2+

+ 94Be → 126C + n

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron5_1.htm

4

2He

2+

+ 94Be → 126C + n

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron5_1.htm

Ionizing Radiation - Interaction with Matter As ionizing radiation moves from point to point in matter, it loses its energy through various interactions with the atoms it encounters. The rate at which this energy loss occurs depends upon the type and energy of the radiation and the density and atomic composition of the matter through which it is passing.

The various types of ionizing radiation impart their energy to matter primarily through excitation and ionization of orbital electrons. The term "excitation" is used to describe an interaction where electrons acquire energy from a passing charged particle but are not removed completely from their atom.

Excited electrons may subsequently emit energy in the form of x-rays during the process of returning to a lower energy state. The term "ionization" refers to the complete removal of an electron from an atom following the transfer of energy from a passing charged particle. In describing the intensity of ionization, the term "specific ionization" is often used. This is defined as the number of ion pairs formed per unit path length for a given type of radiation.

Keywords: Excitation, Ionization, specific ionization.

Charlie Chong/ Fion Zhang

Because of their double charge and relatively slow velocity, alpha particles have a high specific ionization and a relatively short range in matter (a few centimeters in air and only fractions of a millimeter in tissue). Beta particles have a much lower specific ionization than alpha particles and, generally, a greater range. For example, the relatively energetic beta particles from P32 have a maximum range of 7 meters in air and 8 millimeters in tissue. The low energy betas from H3, on the other hand, are stopped by only 6 millimeters of air or 6 micrometers of tissue "specific ionization" is often used.

This is defined as the number of ion pairs formed per unit path length for a given type of radiation.

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Gamma-rays, x-rays, and neutrons are referred to as indirectly ionizing radiation since, having no charge, they do not directly apply impulses to orbital electrons as do alpha and beta particles. Electromagnetic radiation proceed through matter until there is a chance of interaction with a particle. If the particle is an electron, it may receive enough energy to be ionized, whereupon it causes further ionization by direct interactions with other electrons. As a result, indirectly ionizing radiation (e.g. gamma, x-rays, and neutrons) can cause the liberation of directly ionizing particles (electrons) deep inside a medium. Because these neutral radiations undergo only chance encounters with matter, they do not have finite ranges, but rather are attenuated in an exponential manner. In other words, a given gamma ray has a definite probability of passing through any medium of any depth.

Keywords: directly ionizing radiation – Beta, Alpha particle. indirectly ionizing radiation – γ ray, X-ray, neutron particle.

Charlie Chong/ Fion Zhang

Neutrons lose energy in matter by collisions which transfer kinetic energy.

This process is called moderation and is most effective if the matter the neutrons collide with has about the same mass as the neutron.

Once slowed down to the same average energy as the matter being interacted with (thermal energies), the neutrons have a much greater chance of interacting with a nucleus. Such interactions can result in material becoming radioactive or can cause radiation to be given off.

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The quantity which expresses the degree of radioactivity or radiation producing potential of a given amount of radioactive material is activity.

The concentration of radioactivity, or the relationship between the mass of radioactive material and the activity, is called "specific activity." Specific activity is expressed as the number of curies or becquerels per unit mass or volume. â– Each gram of Cobalt-60 will contain approximately 50 curies. â– Each gram of Iridium-192 will contain approximately 350 curies.

The shorter half-life, the less amount of material that will be required to produce a given activity or curies. The higher specific activity of Iridium results in physically smaller sources This allows technicians to place the source in closer proximity to the film while maintaining geometric unsharpness requirements on the radiograph. These unsharpness requirements may not be met if a source with a low specific activity were used at similar source to film distances.

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

Extra curriculum

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Neutron

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Quarks Neutrons and Protons – do they have a structure?

As early as 1961 a paper appeared in Discovery magazine by Professor EHS Burhop of University College London suggesting that protons and neutrons were in fact not fundamental particles but that they had a structure. In 1964 Murray Gell-Mann and George Zweig proposed that all hadrons (mesons and baryons) were composed of particles that they called QUARKS. These were finally discovered in 1975 and at the present time (2002) are thought to be the fundamental particles of matter. One of the most unusual properties of quarks is that they have fractional electric charge compared with the charge on the electron of -e.

Their existence was confirmed by high energy electron scattering from the nucleons.

There are actually six quarks and their anti-quarks but in every day life we are only concerned with three types: the up quark, the down quark and the strange quark. (other quarks are charm, top and bottom) Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

Properties of quarks

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

Quarks in protons and neutrons It was found that quarks can only exit in threes in a proton or neutron. They are held together to form a larger particle by the strong force produced by the exchange of gluons between them. These particles contain three quarks. It has proved very difficult if not impossible to obtain an isolated quark. As you try to pull them out of the proton or neutron it gets more and more difficult.

Even stranger is the suggestion that if you could pull a quark out of a proton it would immediately form a quark- antiquark pair and leave you with a quark inside the proton and nothing outside – status quo!

The reason that it is impossible to get a quark "on its own" is because as you try to separate them from each other the energy needed gets greater and greater. In fact when they "break apart" the energy is sufficient to create two new antiquarks and these join to form pions and so the quarks "disappear"!

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

Quark composition of baryons including the proton and the neutron

All baryons and antibaryons are made up of three quarks.

Proton: up up down uud charge = +2/3 +2/3 -1/3 = +1 Neutron: down down up ddu charge = -1/3 -1/3 +2/3 = 0 Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

You must be careful that you are clear of what diagrams that show three quarks IN a proton or a neutron are supposed to explain. The three quarks ARE the proton or the neutron but the drawings just help to show this.

Notice that electrons and neutrinos contain no quarks, they are themselves truly fundamental particles (or so we think at present) When you try and drag a quark out of a proton the strong force gets bigger and bigger – rather like the force in a spring as it is stretched.

The "mass" of the up and down quarks is 360 MeV. Three of them in a proton gives a mass of 1080 MeV. The mass of the proton is around 930 MeV giving a sort of binding energy of 150 MeV.

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

The quark nature of beta decay The quark nature of the proton and neutron can be used to explain beta decay.

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

Quark version: In beta plus decay an up quark changes into down quark with the emission of a positron and a neutrino, while in beta minus decay a down quark changes into a up quark with the emission of an electron and an anti-neutrino.

The quarks are held together in the nucleus by the strong nuclear force. This acts only over a very short range, around 10-15 m and is also responsible for holding the neutrons and protons together in the nucleus. It is thought that the force is carried by the exchange of virtual particles called gluons! These are allowed to appear and disappear as long as they do not violate Heisenberg's uncertainty principle.

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

This means that the particle can exist for a time of Δt as long as its energy is no greater than (h/2π)/Δt or more usefully it can have an energy of ΔE as long as it exits for less than (h/2π)/ΔE where h is Plank's constant (6.64x10-34 Js).

Additional note – mesons and baryons Baryons are composed of three quarks while mesons are composed of two quarks. One of the quarks in any meson is an anti-quark. For example a π+ meson is composed of one up quark and one anti-down quark.

Charlie Chong/ Fion Zhang

http://schoolphysics.co.uk/age16-19/Nuclear%20physics/Nuclear%20structure/text/Quarks_/index.html

What is inside the nucleus?

By 1910 the atom was thought to consist of a massive nucleus orbited by electrons, but measurements of atomic mass indicated that all nuclei must contain integer numbers of some other particle. What were these particles inside the nucleus?

One of these particles was the proton. The proton was discovered during investigations of positive rays, and can be produced by ionising hydrogen.

Hydrogen is the lightest type of atom, consisting of a single proton and a single electron. Ionisation separates the electron from the atom, so only the proton remains.

If more massive nuclei contained only protons their charge would be much higher than measurements suggested. With the exception of hydrogen all atoms have a higher mass number than charge number. Rutherford thought that the nucleus consisted of protons and 'neutral doublets' formed from closely bound protons and electrons. This could explain both the mass and the charge that had been measured for different nuclei.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Chadwick's neutron chamber containing parallel disks of radioactive polonium and beryllium. Radiation is emitted from an aluminium window at the chamber's end

aluminium window

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

James Chadwick (20 October 1891 – 24 July 1974) Charlie Chong/ Fion Zhang

2. The elusive neutron Rutherford described his 'neutral doublet', or neutron, in 1920. The particle would be uncharged but with a mass only slightly greater than the proton.

Because it was uncharged there would be no electrical repulsion of the neutron as it passed through matter, so it would be much more penetrating than the proton. This would make the neutron difficult to detect.

The discovery of the neutron was made by James Chadwick, who spent more than a decade searching. Chadwick had accompanied Rutherford in his move from Manchester to Cambridge. He later became the Assistant Director of Research in the Cavendish, and was responsible for keeping Rutherford informed of any new developments in physics. Chadwick and Rutherford often discussed neutrons, and suggested 'silly' experiments to discover them, but the inspiration for Chadwick's discovery came from Europe, not Rutherford.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Proton & Neutron Passing Thru Matters

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

3. Beryllium radiation In 1930 the German physicists Bothe and Becker bombarded the light metal beryllium with alpha particles, and noticed that a very penetrating radiation was emitted. This radiation was non-ionising, and they assumed it was gamma rays.

In 1932 Irène and Frédéric Joliot-Curie investigated this radiation in France.

They let the radiation hit a block of paraffin wax, and found it caused the wax to emit protons. They measured the speeds of these protons and found that the gamma rays would have to be incredibly energetic to knock them from the wax.

Chadwick reported the Joliot-Curie's experiment to Rutherford, who did not believe that gamma rays could account for the protons from the wax. He and Chadwick were convinced that the beryllium was emitting neutrons. Neutrons have nearly the same mass as protons, so should knock protons from a wax block fairly easily.

4

2He

2+

+ 94Be → 126C + 10n0

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Ernest Rutherford

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Charlie Chong/ Fion Zhang

4. Chadwick's discovery Chadwick worked day and night to prove the neutron theory, studying the beryllium radiation with an ionisation counter and a cloud chamber. He found that the wax could be replaced with other light substances, even beryllium, and that protons were still produced. Within a month Chadwick had conclusive proof of the existence of the neutron. He published his findings in the journal, Nature, on February 27, 1932.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Chadwick’s Experiment

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

5. Neutrons from beryllium The alpha-particles from the radioactive source hit the beryllium nuclei and transformed them into carbon nuclei, leaving one free neutron. When this neutron hit the hydrogen nuclei in the wax it could knock a proton free, in the same way that a white snooker ball can transfer all its energy to a red snooker ball.

Rutherford gave the best description of a neutron as a highly penetrating neutral particle with a mass similar to the proton. We now know it is not a combination of an electron and a proton. Quantum mechanics restricts an electron from getting that close to the proton, and measurements of nuclear 'spin' provide experimental proof that the nucleus does not contain electrons.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

tank erections whereby

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

6. The decaying particle Chadwick knew the neutron wasn't formed from an electron and a proton, and explained in his Nobel lecture that it seemed 'useless to discuss whether the neutron and proton are elementary particles or not'. He knew that a more powerful investigation of the neutron was necessary to decide if it was made up of anything else. We now believe that the neutron and the proton are made of even tinier particles called quarks.

To further confuse matters, free neutrons are not stable. If a neutron is outside the nucleus for several minutes it will transform into a proton, an electron, and an extremely light particle called a neutrino. The decay occurs because one of the quarks inside the neutron has transformed into a different quark, producing an additional positive charge in the particle.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

7. The nuclear bomb Neutrons are very penetrating because they are uncharged. This makes them very useful to nuclear physicists, as they can be fired into the nucleus without being repelled like the proton. A neutron can even be made to stop inside a nucleus, transforming elements into more massive types.

This understanding of the neutron allowed scientists to develop nuclear power, and nuclear weapons during the Second World War. Chadwick helped in the theory behind the first nuclear bombs, and used a particle accelerator in Liverpool to show that it is possible to construct them with only a few kilograms of uranium.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

This short video clip shows the 'Trinity' nuclear fission bomb, tested in the desert of New Mexico, USA on July 16, 1945. Three weeks later America dropped two similar bombs, using different fissile material, on Japan. The Trinity bomb was the first nuclear fission explosion on Earth and resulted in a blast that could be felt over 250 miles away. The Trinity bomb used plutonium as its fissile material, the same metal used in the bomb dropped on Nagasaki.

The Hiroshima bomb used the slightly lighter metal uranium.

Charlie Chong/ Fion Zhang

http://www-outreach.phy.cam.ac.uk/camphy/neutron/neutron1_1.htm

Trinity Nuclear Fission Bomb

Charlie Chong/ Fion Zhang

http://nuclearweaponarchive.org/Usa/Tests/Trinity.html

http://www.dailymail.co.uk/news/article-2645299/Haunting-photographs-Nagasaki-wake-atomic-bomb-attack-used-Japanese-propaganda-stolen-U-S-soldier.html

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang http://www.dailymail.co.uk/news/article-2645299/Haunting-photographs-Nagasaki-wake-atomic-bomb-attack-used-Japanese-propaganda-stolen-U-S-soldier.html

Charlie Chong/ Fion Zhang

http://www.dailymail.co.uk/news/article-2645299/Haunting-photographs-Nagasaki-wake-atomic-bomb-attack-used-Japanese-propaganda-stolen-U-S-soldier.html

http://www.dailymail.co.uk/news/article-2645299/Haunting-photographs-Nagasaki-wake-atomic-bomb-attack-used-Japanese-propaganda-stolen-U-S-soldier.html

Charlie Chong/ Fion Zhang

Reading is always fun! End of Reading

Charlie Chong/ Fion Zhang

The neutron is a subatomic particle, symbol n or n0, with no net electric charge and a mass slightly larger than that of a proton. Protons and neutrons, each with mass approximately one atomic mass unit, constitute the nucleus of an atom, and they are collectively referred to as nucleons. Their properties and interactions are described by nuclear physics.

The nucleus consists of Z protons, where Z is called the atomic number, and N neutrons, where N is the neutron number. The atomic number defines the chemical properties of the atom, and the neutron number determines the isotope or nuclide. The terms isotope and nuclide are often used synonymously, but they refer to chemical and nuclear properties, respectively.

The atomic mass number, symbol A, equals Z+N. For example, carbon has atomic number 6, and its abundant carbon-12 isotope has 6 neutrons, whereas its rare carbon-13 isotope has 7 neutrons. Some elements occur in nature with only one stable isotope, such as fluorine. Other elements occur as many stable isotopes, such as tin with ten stable isotopes. Even though it is not a chemical element, the neutron is included in the table of nuclides.

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Within the nucleus, protons and neutrons are bound together through the nuclear force, and neutrons are required for the stability of nuclei. Neutrons are produced copiously in nuclear fission and fusion. They are a primary contributor to the nucleosynthesis of chemical elements within stars through fission, fusion, and neutron capture processes.

The neutron is essential to the production of nuclear power. In the decade after the neutron was discovered in 1932, neutrons were used to effect many different types of nuclear transmutations. With the discovery of nuclear fission in 1938, it was quickly realized that, if a fission event produced neutrons, each of these neutrons might cause further fission events, etc., in a cascade known as a nuclear chain reaction. These events and findings led to the first self-sustaining nuclear reactor (Chicago Pile-1, 1942) and the first nuclear weapon (Trinity, 1945).

Charlie Chong/ Fion Zhang

Free neutrons, or individual neutrons free of the nucleus, are effectively a form of ionizing radiation, and as such, are a biological hazard, depending upon dose. A small natural "neutron background" flux of free neutrons exists on Earth, caused by cosmic ray showers, and by the natural radioactivity of spontaneously fissionable elements in the Earth's crust. Dedicated neutron sources like neutron generators, research reactors and spallation sources produce free neutrons for use in irradiation and in neutron scattering experiments.

Charlie Chong/ Fion Zhang

Chapter 2: Newton's Inverse Square Law Any point source which spreads its influence equally in all directions without a limit to its range will obey the inverse square law. This comes from strictly geometrical considerations. The intensity of the influence at any given radius (r) is the source strength divided by the area of the sphere. Being strictly geometric in its origin, the inverse square law applies to diverse phenomena. Point sources of gravitational force, electric field, light, sound, or radiation obey the inverse square law. As one of the fields which obey the general inverse square law, a point radiation source can be characterized by the diagram above whether you are talking about Roentgens, rads, or rems.

All measures of exposure will drop off by the inverse square law. For example, if the radiation exposure is 100 mR/hr at 1 inch from a source, the exposure will be 0.01 mR/hr at 100 inches.

Charlie Chong/ Fion Zhang

Inverse Square Law

Charlie Chong/ Fion Zhang

Isotope Decay Rate Gamma-rays are electromagnetic radiation emitted by the disintegration of a radioactive isotope and have energy from about 100 keV to well over 1 MeV, corresponding to about 0.01 to 0.001 Å. The most useful gamma-emitting radioactive isotopes for radiological purposes are found to be cobalt (Co60), iridium (Ir192), cesium (Cs137), ytterbium (Yb169), and thulium (Tm170).

N(t) = Noe –λt Decay Rate:  dN/dt ∝N  dN/dt = -λN  ∫dN/N = ∫-λdt  ln N +C’ = -λt + C″  ln N = -λt + C  N = e-λt · eC

Charlie Chong/ Fion Zhang

When t = 0  N = No = eC  N = Noe -λt  When N=1/2No, t= T½  0.5 = e –λT ½  ln 0.5 = –λT½  λ = 0.693/T ½  N = Noe -0.693t/T½

http://chemwiki.ucdavis.edu/Core/Physical_Chemistry/Nuclear_Chemistry/Radioactivity/Radioactive_Decay_Rates

Carbon-14 Dating

Charlie Chong/ Fion Zhang

Radio-carbon dating is a method of obtaining age estimates on organic materials which has been used to date samples as old as 50,000 years. The method was developed immediately following World War II by Willard F. Libby and coworkers and has provided age determinations in archeology, geology, geophysics, and other branches of science. Radiocarbon determinations can be obtained on wood, charcoal, marine and freshwater shell, bone and antler, and peat and organic-bearing sediments. They can also be obtained from carbonate deposits such as tufa, calcite, marl, dissolved carbon dioxide, and carbonates in ocean, lake and groundwater sources.

Each sample type has specific problems associated with its use for dating purposes, including contamination and special environmental effects. While the impact of radiocarbon dating has been most profound in archeological research and particularly in prehistoric studies, extremely significant contributions have also been made in hydrology and oceanography. In addition, in the 1950's the testing of thermonuclear weapons injected large amounts of artificial radiocarbon ("Radiocarbon Bomb") into the atmosphere, permitting it to be used as a geochemical tracer.

Charlie Chong/ Fion Zhang

Carbon dioxide is distributed on a worldwide basis into various atmospheric, biospheric, and hydrospheric reservoirs on a time scale much shorter than its half-life. Metabolic processes in living organisms and relatively rapid turnover of carbonates in surface ocean waters maintain radiocarbon levels at approximately constant levels in most of the biosphere.

Most living organisms absorb carbon. During its lifetime, an organism continually replenishes its supply of carbon just by breathing and eating.

Carbon (C) has three naturally occurring isotopes. Both C-12 and C-13 are stable, but C-14 decays by very weak beta decay to nitrogen-14 with a halflife of approximately 5,730 years. Naturally occurring Radiocarbon is produced as a secondary effect of cosmic-ray bombardment of the upper atmosphere.

Charlie Chong/ Fion Zhang

After the organism dies and becomes a fossil, Carbon-14 continues to decay without being replaced. To measure the amount of radiocarbon left in a fossil, scientists burn a small piece to convert it into carbon dioxide gas. Radiation counters are used to detect the electrons given off by decaying C-14 as it turns into nitrogen. The amount of C-14 is compared to the amount of C-12, the stable form of carbon, to determine how much radiocarbon has decayed, therefore, dating the fossil.

N = Noe-λt = Noe -0.693t/T½ Where “N" is the present amount of the radioactive isotope, “No" is the original amount of the radioactive isotope that is measured in the same units as "A." "t" is the time it takes to reduce the original amount of the isotope to the present amount, and “ T½" is the half-life of the isotope, measured in the same units as "t."

Charlie Chong/ Fion Zhang

t has long been recognized that if radiocarbon atoms could be detected directly, rather than by waiting for their decay, smaller samples could be used for dating and older dates could be measured. A simple hypothetical example to illustrate this point is a sample containing only one atom of radiocarbon. To measure the age (that is, the abundance of radiocarbon), the sample can be placed into a mass spectrometer and that atom counted, or the sample can be placed into a Geiger counter and counted, requiring a wait on the average of 8,000 years (the mean life of radiocarbon) for the decay. In practice, neither the atoms nor the decays can be counted with 100% efficiency.

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Chapter 3 Interaction Between Penetrating Radiation and Matter Interaction between penetrating radiation and matter is not a simple process in which the primary x-ray photon changes to some other form of energy and effectively disappears. The diagram below shows the absorption coefficient, Âľ, for four radiation-matter interactions as a function of radiation energy in MeV. The graph is representative of radiation interacting with Iron. Absorption will be covered in greater detail in a later page.

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Summary of different mechanisms that reduce intensity of an incident x-ray beam Photoelectric (PE) absorption of x-rays occurs when the x-ray photon is absorbed resulting in the ejection of electrons from the outer shell of the atom, resulting in the ionization of the atom. Subsequently, the ionized atom returns to the neutral state with the emission of an x-ray characteristic of the atom.

This subsequent emission of lower energy photons is generally absorbed and does not contribute to (or hinder) the image making process. Photoelectron absorption is the dominant process for x-ray absorption up to energies of about 500 KeV. Photoelectron absorption is also dominant for atoms of high atomic numbers.

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Photoelectric

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Pair Production (PP) can occur when the x-ray photon energy is greater than 1.02 MeV, when an electron and positron are created with the annihilation of the x-ray photon. Positrons are very short lived and disappear (positron annihilation) with the formation of two photons of 0.51 MeV energy.

Pair production is of particular importance when high-energy photons pass through materials of a high atomic number. Energy: > 1.02 MeV

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Compton Scattering (C), also known a incoherent scattering, occurs when the incident x-ray photon ejects a electron from an atom and an x-ray photon of lower energy is scattered from the atom. Relativistic energy and momentum are conserved in this process (demonstrated in the applet below) and the scattered x-ray photon has less energy and therefore greater wavelength than the incident photon. Compton Scattering is important for low atomic number specimens. At energies of 100 keV -- 10 MeV the absorption of radiation is mainly due to the Compton effect.

Charlie Chong/ Fion Zhang

Together with the scattering of photons on free electrons, the photoelectric effect, and pair production, Compton scattering contributes to the attenuation of x-rays in matter. As the binding energy of electrons in atoms is low compared to that of passing near-relativistic particles, this is the relevant process in radiography. Closely related are Thompson scattering (classical treatment of photon scattering) and Rayleigh scattering (coherent scattering on atoms).

Compton Scattering, also known as incoherent scattering, occurs when the incident x-ray photon ejects a electron from an atom and an x-ray photon of lower energy is scattered from the atom. Relativistic energy and momentum are conserved in this process (demonstrated in the applet below) and the scattered x-ray photon has less energy and therefore a longer wavelength than the incident photon. Compton scattering is important for low atomic number specimens.

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Below are other interaction phenomenon that can occur. Under special circumstances these may need to be considered, but are generally negligible.

Thomson scattering (R), also known as Rayleigh, coherent, or classical scattering, occurs when the x-ray photon interacts with the whole atom so that the photon is scattered with no change in internal energy to the scattering atom, nor to the x-ray photon. Thomson scattering is never more than a minor contributor to the absorption coefficient. The scattering occurs without the loss of energy. Scattering is mainly in the forward direction.

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

http://www.mssl.ucl.ac.uk/www_astro/lecturenotes/hea/radprocess/sld001.htm

Idea of Cross Section: In nuclear and particle physics, the concept of a neutron cross section is used to express the likelihood of interaction between an incident neutron and a target nucleus. In conjunction with the neutron flux, it enables the calculation of the reaction rate, for example to derive the thermal power of a nuclear power plant. The standard unit for measuring the cross section is the barn, which is equal to 10−28 m2 or 10−24 cm2. The larger neutron cross section, the more likely a neutron will react with the nucleus.

Charlie Chong/ Fion Zhang

Photodisintegration (PD) is the process by which the x-ray photon is captured by the nucleus of the atom with the ejection of a particle from the nucleus when all the energy of the x-ray is given to the nucleus. Because of the enormously high energies involved, this process may be neglected for the energies of x-rays used in radiography.

Example: 9Be + >1.7 Mev photon → 1 neutron + 4He 2 2H (deuterium) + >2.26 MeV photon → 1 neutron + 1H https://en.wikipedia.org/wiki/Neutron_source

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

http://www.kuwo.cn/yinyue/302998/

Charlie Chong/ Fion Zhang

https://www.youtube.com/watch?v=3fLuPIPp0p4

Charlie Chong/ Fion Zhang

https://www.youtube.com/watch?v=3fLuPIPp0p4

Charlie Chong/ Fion Zhang

https://www.youtube.com/watch?v=3fLuPIPp0p4

Chapter 4 Absorption Absorption characteristics of materials are important in the development of contrast in a radiograph. Absorption characteristics will increase or decrease as the energy of the x-ray is increased or decreased. A radiograph with higher contrast will provide greater probability of detection of a given discontinuity.

An understanding of the relationship between material thickness, absorption properties, and photon energy is fundamental to producing a quality radiograph. An understanding of absorption is also necessary when designing x- and gamma ray shielding, cabinets, or exposure vaults.

Attenuation of x-rays in solids takes place by several different mechanisms, some due to absorption, others due to the scattering of the beam. Thompson scattering (also known as Rayleigh, coherent, or classical scattering) and Compton Scattering (also known as incoherent scattering) were introduced in the material titled "Interaction Between Penetrating Radiation and Matter" and "Compton Scattering." This needs careful attention because a good radiograph can only be achieved if there is minimum x-ray scattering.

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The figure below shows an approximation of the Absorption coefficient, Âľ, in red, for Iron plotted as a function of radiation energy.

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The attenuation or absorption, usually defined as the linear absorption coefficient, Âľ, is defined for a (1) narrow well-collimated, (2) monochromatic x-ray beam. The linear absorption coefficient is the sum of contributions of the following: 1. Thomson scattering (R) (also known as Rayleigh, coherent, or classical scattering) occurs when the x-ray photon interacts with the whole atom so that the photon is scattered with no change in internal energy to the scattering atom, nor to the x-ray photon.

2. Photoelectric (PE) absorption of x-rays occurs when the x-ray photon is absorbed resulting in the ejection of electrons from the outer shell (?) of the atom, resulting in the ionization of the atom. Subsequently, the ionized atom returns to the neutral state with the emission of an x-ray characteristic of the atom.

3. Compton Scattering (C) (also known a incoherent scattering) occurs when the incident x-ray photon ejects an electron from an atom and a x-ray photon of lower energy is scattered from the atom.

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4. Pair Production (PP) can occur when the x-ray photon energy is greater than 1.02 MeV, when an electron and positron are created with the annihilation of the x-ray photon (absorption).

5. Photodisintegration (PD) is the process by which the x-ray photon is captured by the nucleus of the atom with the ejection of a particle from the nucleus when all the energy of the x-ray is given to the nucleus (absorption). This process may be neglected for the energies of x-rays used in radiography. (>10Mev?)

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A narrow beam of monoenergetic photons with an incident intensity Io, penetrating a layer of material with mass thickness x and density p, emerges with intensity I given by the exponential attenuation law,

I/Io = e -(Âľ/p)x which can be rewritten as:

Âľ/p = ln(Io/I)/x from which can be obtained from measured values of Io, I and x. Note that the mass thickness is defined as the mass per unit area, and is obtained by multiplying the thickness t by the density, i.e., x = t. These conditions, generally do not apply to radiography. Scattered x-rays leave the beam and and contribute to the decrease in intensity.

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Geometry and X-ray Resolution Source to film distance, object to film distance, and source size directly affect the degree of penumbra shadow and geometric unsharpness of a radiograph. Codes and standards used in industrial radiography require that geometric unsharpness be limited.

The three factors controlling unsharpness are source size, source to object distance, and object to detector distance. The source size is obtained by referencing manufacturers specifications for a given x- or gamma ray source. Industrial x-ray tubes often have source (anode) sizes of 1.5 mm2. A balance must be maintained between duty cycle, killovoltage applied, and source size. X-ray sources (anodes) may be reduced to sizes as small as microns for special applications. As the source (anode) size is increased or decreased, distance to the object can be increased or decreased and geometric unsharpness will remain constant. Source to object distance is primarily dependent on source size. Object to detector (object to film) distance is maintained as close as the particle. If the object is suspended above the detector an increase in unsharpness will result. Another result of the object being some distance from the film is geometric enlargement. This technique is used on small components. Industrial radiographers will use an externally small source and the object suspended above the detector that produces an enlarged image on the radiograph. Radiography of transistors and computer chips is one application of this technique.

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Charlie Chong/ Fion Zhang

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Additionally, it is generally accepted that an x-ray beam's intensity is not uniform throughout its entirety. Illustrated at the right, as x-radiation is emitted from the target area in a conical shape, measurements have determined that the intensity in the direction of the anode (AC) is lower (over and above the difference caused by the Inverse Square Law)

anode

C

A

B

than the intensity in the direction of the cathode (AB). The fact that the intensities vary in such a manner causes visible differences in the density produced on the radiographs. This phenomenon is called heel effect.

Radiographers should be aware of this phenomenon as codes require a minimum density through the area of interest. On low density radiographs the heal effect could cause a portion of the radiograph to not meet these requirements.

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The decreased intensity at "C" results from emission which is nearly parallel to the angled target where there is increasing absorption of the x-ray photons by the target itself (?) . This phenomenon is readily apparent in rotating anode tubes because they utilize steeply angled anodes of generally 17 degrees or less. Generally, the steeper the anode, the more severe or noticeable the heel effect becomes.

The greater the focus film distance, the less noticeable the heel effect due to the smaller cone of radiation used to cover a given area. Heel effect is less significant on small films. This is due to the fact that the intensity of an x-ray beam is much more uniform near the central ray.

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C

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A

B

Rotating Anode Tube

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http://www.orau.org/ptp/collection/xraytubescoolidge/xraytubescoolidge.htm

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http://www.orau.org/ptp/collection/xraytubescoolidge/xraytubescoolidge.htm

Filters in Radiography At x-ray energies, filters consist of material placed in the useful beam to absorb, preferentially, radiations based on energy level or to modify the spatial distribution of the beam. Filtration is required to absorb the lowerenergy x-ray photons emitted by the tube before they reach the target. The use of filters produce a cleaner image by absorbing the lower energy x-ray photons that tend to scatter more.

The total filtration of the beam includes the inherent filtration (composed of part of the x-ray tube and tube housing) and the added filtration (thin sheets of a metal inserted in the x-ray beam). Filters are typically placed at or near the x-ray port in the direct path of the x-ray beam. Placing a thin sheet of copper between the part and the film cassette has also proven an effective method of filtration.

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For industrial radiography, the filters added to the x-ray beam are most often constructed of high atomic number materials such as lead, copper, or brass.

Filters for medical radiography are usually made of aluminum (Al). The amount of both the inherent and the added filtration are stated in mm of Al or mm of Al equivalent. The amount of filtration of the x-ray beam is specified by and based on the kVp used to produce the beam. The thickness of filter materials is dependent on atomic numbers, kilovoltage settings, and the desired filtration factor.

Gamma radiography produces relatively high energy levels at essentially monochromatic radiation, therefore filtration is not a useful technique and is seldom used.

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Charlie Chong/ Fion Zhang

Secondary (Scatter) Radiation and Undercut Control Secondary or scatter radiation must often be taken into consideration when producing a radiograph. The scattered photons create a loss of contrast and definition. Often secondary radiation is thought of as radiation striking the film reflected from an object in the immediate area, such as a wall, or from the table or floor where the part is resting. Side scatter originates from walls, or objects on the source side of the film. Control of side scatter can be achieved by moving objects in the room away from the film, moving the x-ray tube to the center of the vault, or placing a collimator at the exit port thus reducing the diverging radiation surrounding the central beam.

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

It is often called back scatter when it comes from objects behind the film.

Industry codes and standards often require that a lead letter "B" be placed on the back of the cassette to verify the control of back scatter. If the letter "B" shows as a “ light ghost" image on the film the letter has absorbed the back scatter radiation indicating a significant amount of radiation reaching the film.

Control of back scatter radiation is achieved by backing the film in the cassette with sheets of lead typically 0.010 inch thick.

It is a common practice in industry to place 0.005 lead screen in front and 0.010 backing the film.

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Back Scatter

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https://www.nde-ed.org/TeachingResources/teachingresources.htm

Undercut Another condition that must often be controlled when producing a radiograph is called undercut. Parts with holes, hollow areas, or abrupt thickness changes are likely to suffer from undercut if controls are not put in place.

Undercut appears as lightening of the radiograph in the area of the thickness transition. This results in a loss of resolution or blurring at the transition area.

Undercut occurs due to scattering within the film. At the edges of a part or areas where the part transitions from thick to thin, the intensity of the radiation reaching the film is much greater than in the thicker areas of the part. The high level of radiation intensity reaching the film results in a high level of scattering within the film. It should also be noted that the faster the film speed, the more undercut that is likely to occur. Scattering from within the walls of the part also contributed some to undercut but research has shown that scattering within the film is the primary cause. Masks are used to control undercut. Sheets of lead cut to fill holes or surround the part and metallic shot and liquid absorbers are often used as masks.

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Undercut

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Radiation Safety

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Radiation Safety Radionuclides in various chemical and physical forms have become extremely important tools in modern research. The ionizing radiation emitted by these materials, however, can pose a hazard to human health. For this reason, special precautions must be observed when radionuclides are used.

The possession and use of radioactive materials in the United States is governed by strict regulatory controls. The primary regulatory authority for most types and uses of radioactive materials is the federal Nuclear Regulatory Commission (NRC). However, more than half of the states in the US (including Iowa) have entered into "agreement" with the NRC to assume regulatory control of radioactive material use within their borders. As part of the agreement process, the states must adopt and enforce regulations comparable to those found in Title 10 of the Code of Federal Regulations.

Regulations for control of radioactive material use in Iowa are found in Chapter 136C of the Iowa Code.

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For most situations, the types and maximum quantities of radioactive materials possessed, the manner in which they may be used, and the individuals authorized to use radioactive materials are stipulated in the form of a "specific" license from the appropriate regulatory authority. In Iowa, this authority is the Iowa Department of Public Health. However, for certain institutions which routinely use large quantities of numerous types of radioactive materials, the exact quantities of materials and details of use may not be specified in the license.

Instead, the license grants the institution the authority and responsibility for setting the specific requirements for radioactive material use within its facilities. These licensees are termed "broadscope" and require a Radiation Safety Committee and usually a full-time Radiation Safety Officer.

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The quantity which expresses the degree of radioactivity or radiation producing potential of a given amount of radioactive material is activity. The special unit for activity is the curie (Ci) which was originally defined as that amount of any radioactive material which disintegrates at the same rate as one gram of pure radium. The curie has since been defined more precisely as a quantity of radioactive material in which 3.7 x 1010 atoms disintegrate per second.

The International System (SI) unit for activity is the becquerel (Bq), which is that quantity of radioactive material in which one atom is transformed per second. The activity of a given amount of radioactive material not depend upon the mass of material present. For example, two one-curie sources of Cs-137 might have very different masses depending upon the relative proportion of non radioactive atoms present in each source. The concentration of radioactivity, or the relationship between the mass of radioactive material and the activity, is called the specific activity. Specific activity is expressed as the number of curies or becquerels per unit mass or volume.

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The concentration of radioactivity, or the relationship between the mass of radioactive material and the activity, is called the specific activity. Specific activity is expressed as the number of curies or becquerels per unit mass or volume.

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

Chapter 5 Radiation Safety Radionuclides in various chemical and physical forms have become extremely important tools in modern research. The ionizing radiation emitted by these materials, however, can pose a hazard to human health. For this reason, special precautions must be observed when radionuclides are used.

The possession and use of radioactive materials in the United States is governed by strict regulatory controls. The primary regulatory authority for most types and uses of radioactive materials is the federal Nuclear Regulatory Commission (NRC). However, more than half of the states in the US (including Iowa) have entered into "agreement" with the NRC to assume regulatory control of radioactive material use within their borders. As part of the agreement process, the states must adopt and enforce regulations comparable to those found in Title 10 of the Code of Federal Regulations.

Regulations for control of radioactive material use in Iowa are found in Chapter 136C of the Iowa Code.

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Charlie Chong/ Fion Zhang

ABSORBED DOSE - RAD (Radiation Absorbed Dose) The absorbed dose is the quantity that expresses the amount of energy which ionizing radiation imparts to a given mass of matter.

1. The special unit for absorbed dose is the RAD (Radiation Absorbed Dose), which is defined as a dose of 100 ergs of energy per gram of matter.

2. The SI unit for absorbed dose is the gray (Gy), which is defined as a dose of one joule per kilogram.

3. Since one joule equals 107 ergs, and since one kilogram equals 1000 grams, 1 Gray equals 100 rads.

The size of the absorbed dose is dependent upon the strength (or activity) of the radiation source, the distance from the source to the irradiated material, and the time over which the material is irradiated. The activity of the source will determine the dose rate which can be expressed in rad/hr, mrad/hr, mGy/sec, etc. (mGy/sec/m?)

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Charlie Chong/ Fion Zhang

DOSE EQUIVALENT - REM (Roentgen Equivalent Man) Although the biological effects of radiation are dependent upon the absorbed dose, some types of particles produce greater effects than others for the same amount of energy imparted. For example, for equal absorbed doses, alpha particles may be 20 times as damaging as beta particles. In order to account for these variations when describing human health risk from radiation exposure, the quantity called dose equivalent is used. This is the absorbed dose multiplied by certain "quality" and "modifying" factors (QF) indicative of the relative biological damage potential of the particular type of radiation.

The special unit for dose equivalent is the rem (Roentgen Equivalent Man).

The SI unit for dose equivalent is the sievert (Sv).

Keywords: Rongent - dose rate for ionization of dry air at °C Rad (Gray) – dose rate of ionization of 1 joule per kilogram (tissue? Or any matters?)

Rem (Sievert) – Roentgen equivalent man

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Charlie Chong/ Fion Zhang

X-ray Sources

X-rays are just like any other kind of electromagnetic radiation. They can be produced in parcels of energy called photons, just like light. There are two different atomic processes that can produce X-ray photons. One is called Bremsstrahlung and is a German term meaning "braking radiation." The other is called K-shell emission (L-shell?) . They can both occur in the heavy atoms of tungsten. Tungsten is often the material chosen for the target or anode of the x-ray tube.

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Both ways of making X-rays involve a change in the state of electrons.

However, Bremsstrahlung is easier to understand using the classical idea that radiation is emitted when the velocity of the electron shot at the tungsten changes. The negativity charged electron slows down after swinging around the nucleus of a positively charged tungsten atom. This energy loss produces X-radiation. Electrons are scattered elastically and inelastically by the positively charged nucleus. The inelastically scattered electron loses energy, which appears as Bremsstrahlung. Elastically scattered electrons (which include backscattered electrons) are generally scattered through larger angles. In the interaction, many photons of different wavelengths are produced, but none of the photons have more energy than the electron had to begin with. After emitting the spectrum of X-ray radiation the original electron is slowed down or stopped.

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Bremsstrahlung Radiation X-ray tubes produce x-ray photons by accelerating a stream of electrons to energies of several hundred kilovolts with velocities of several hundred kilometers per hour and colliding them into a heavy target material. The abrupt acceleration of the charged particles (electrons) produces Bremsstrahlung photons. X-ray radiation with a continuous spectrum of energies is produced ranging from a few keV to a maximum of energy of the electron beam.

Target materials for industrial tubes are typically tungsten, which means that the wave functions of the bound tungsten electrons are required. The inherent filtration of an X-ray tube must be computed, this is controlled by the amount that the electron penetrates into the surface of the target and by the type of vacuum window present.

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The bremsstrahlung photons generated within the target material are attenuated as they pass out through typically 50 microns of target material.

The beam is further attenuated by the aluminum or beryllium vacuum window.

The results are an elimination of the low energy photons, 1 keV through 15keV, and a significant reduction in the portion of the spectrum from 15 keV through 50 keV. The spectrum from an x-ray tube is further modified by the filtration caused by the selection of filters used in the setup.

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Charlie Chong/ Fion Zhang

http://hyperphysics.phy-astr.gsu.edu/%E2%80%8Chbase/quantum/xtube.html

Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

K-shell emission Radiation Remember that atoms have their electrons arranged in closed "shells" of different energies. The K-shell is the lowest energy state of an atom. An incoming electron can give a K-shell electron enough energy to knock it out of its energy state. About 0.1% of the (incoming accelerated – cathode ray) electrons produce K-shell vacancies; most (99.9%) produce heat. Then, a tungsten electron of higher energy (from an outer shell) can fall into the Kshell. The energy lost by the falling electron shows up in an emitted x-ray photon. Meanwhile, higher energy electrons fall into the vacated energy state in the outer shell, and so on. K-shell emission produces higher-intensity xrays than Bremsstrahlung, and the x-ray photon comes out at a single wavelength.

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K-shell emission Radiation

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When outer-shell electrons drop into inner shells, they emit a quantized photon "characteristic" of the element. The energies of the characteristic Xrays produced are only very weakly dependent on the chemical structure in which the atom is bound, indicating that the nonbonding shells of atoms are the X-ray source. The resulting characteristic spectrum is superimposed on the continuum as shown in the graphs below. An atom remains ionized for a very short time (about 10E-14 second) and thus an atom can be repeatedly ionized by the incident electrons which arrive about every 10E-12 second.

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Charlie Chong/ Fion Zhang

Charlie Chong/ Fion Zhang

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X-ray Interactions with Matters Q1: In which process is matter converted back to energy? a. nuclear reaction b. annihilation reaction c. Compton scatter d. photodisintegration b. annihilation reaction (part of pair production interaction)

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q2: Which of the following interactions has a significant impact on the x-ray image? a. Compton scattering b. coherent scatter c. pair production d. photodisintegration a. Compton scattering Q3: Which of the following interactions with matter results in a radiograph with a long scale of contrast? a. Compton scattering b. coherent scatter c. photoelectric interactions d. photodisintegration a. Compton scattering

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q4: As the angle of deflection is increased from 0ยบ to 180ยบ, ____. a. all energy is imparted to the incident photon b. less energy is imparted to the recoil electron c. greater energy is imparted to the scattered photon d. greater energy is imparted to the recoil electron d. greater energy is imparted to the recoil electron Q5: When x-ray photons interact with matter and change direction, the process is called ____. a. absorption b. scatter c. radiation d. binding energy b. scatter

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q6: As the electrons shells move further from the nucleus, total electron energies ____ and binding energies ____. a. decrease, decrease b. increase, increase c. increase, decrease d. decrease, increase c. increase, decrease Q7: In which element are the inner shell electrons more tightly bound to the nucleus? a. mercury (Z = 80) b. tungsten (Z = 74) c. lead (Z = 82) d. chromium (Z = 24) c. lead (Z = 82)

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q8: During the process of attenuation, ____ of x-ray photons in the beam. a. there is a reduction in the number b. there is a loss of energy c. there is an interaction d. all of the above d. all of the above Q9: When an x-ray passes through matter, it undergoes a process called ____. a. radiation b. filtration c. attenuation d. fluoroscopy b. annihilation reaction

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q10: If 5% of an incident beam is transmitted through a body part, then 95% of that beam was a. scattered. b. attenuated. c. absorbed. d. back-scattered. b.attenuated.

Q11: At energies below 40 keV, the predominant x-ray interaction in soft tissue and bone is ____. a. coherent scatter b. Compton scatter c. photoelectric absorption d. photodisintegration c. photoelectric absorption

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q12: High kVp techniques reduce a. patient dose. b. differential absorption. c. image fog. d. All of the above. a. patient dose.

Q13: Compton interactions, photoelectric absorption, and transmitted x-rays all contribute to ____. a. image fog b. differential absorption c. patient dose d. attenuation b. differential absorption

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q14: X-rays transmitted without interaction contribute to a. photoelectric absorption. b. the radiographic image. c. the image fog. d. beam attenuation. b. the radiographic image.

Q15: A negative contrast agent is ____. a. air b. iodine c. barium d. water a. air

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q16: The use of contrast agents increases the amount of a. differential absorption. b. Compton scatter. c. photoelectric absorption. d. All of the above. d. All of the above.

Q17: Barium is a good contrast agent because of its a. low atomic number. b. high atomic number. c. light color. d. low density. b. high atomic number.

Charlie Chong/ Fion Zhang

https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q18: Attenuation is caused by ____. a. absorption b. scattering c. transmission. d. Both a and b. d. Both a and b.

Q19: Differential absorption is dependent on the a. kVp of the exposure. b. atomic number of the absorber. c. mass density of the absorber. d. All of the above. d. All of the above.

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q20: Because of differential absorption, about ____ of the incident beam from the x-ray tube contributes to the finished image. a.0.5% b.10% c.50% d.95% a.0.5% Q21: Image fog in diagnostic imaging is caused by a. photoelectric absorption. b. Compton scatter. c. pair production. d. All of the above. b. Compton scatter.

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q22: Which has the greatest mass density? a. fat b. soft tissue c. bone d. air c. bone Q23: K-shell binding energy increases with increasing ____. a. mass density b. kVp c. atomic number d. mAs c. atomic number

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q24: When the mass density of the absorber is ____, it results in ____ Compton scatter. a. decreased, increased b. increased, increased c. increased, decreased d. decreased, decreased b.increased, increased Q25: Only at energies above 10 MeV can ____ take place. a. photodisintegration b. pair production c. Compton scatter d. photoelectric absorption a. photodisintegration

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q26: ____ occurs only at the very high energies used in radiation therapy and in nuclear medicine PET imaging. a. Coherent scatter b. Compton scatter c. Photoelectric absorption d. Pair production d.Pair production Q27: There is complete absorption of the incident x-ray photon with a. photoelectric effect. b. Compton interaction. c. pair production. d. coherent scatter. a. photoelectric effect. (pair production only if E = 1.02 Mev exactly)

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q28: As kVp ____, the probability of photoelectric absorption ____. a. increases, remains the same b. increases, decreases c. decreases, decreases d. decreases, remains the same b. increases, decreases Q29: Compton scatter is directed at (a) ____ angle from the incident beam. a. 180ยบ b. 90ยบ c. 0ยบ d. any d.any

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q30: The scattered x-ray from a Compton interaction usually retains ____ of the energy of the incident photon. a. none b. little c. most d. all c. most Q31: Which x-ray interaction involves the ejection of the K-shell electron? a. coherent scattering b. Compton interaction c. pair production d. photoelectric absorption d. photoelectric absorption

Charlie Chong/ Fion Zhang

https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q32: The scattered x-ray from a Compton interaction usually retains ____ of the energy of the incident photon. a. none b. little c. most d. all c.most Q33: Which x-ray interaction involves the ejection of the K-shell electron? a. coherent scattering b. Compton interaction c. pair production d. photoelectric absorption d. photoelectric absorption

Charlie Chong/ Fion Zhang

https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q34: An outer-shell electron is ejected and the atom is ionized with a. photoelectric interactions. b. Compton interactions. c. coherent scattering. d. pair production. b. Compton interactions.

Q35: An incident x-ray interacts with an atom without ionization during ____. a. photoelectric absorption b. Compton scattering c. coherent scattering d. pair production c.coherent scattering (momentarily no ionization?)

Charlie Chong/ Fion Zhang

https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Coherent scatter (or Thompson scatter) There are three main steps in coherent scatter.

1. An incoming x ray photon with less than 10 keV (so a very low energy x ray photon) interacts with an outer orbital electron.

2. The incoming x ray photon transfers ALL of its energy to the outer orbital electron. The incoming x ray photon no longer exists after transferring its energy. This makes the outer orbital electron excited.

3. The outer orbital electron gives off the excess energy (in the form of an x ray photon) in a different direction than the original incoming x ray photon.

The new x ray photon has the same energy as the incoming x ray photon.

Charlie Chong/ Fion Zhang

http://drgstoothpix.com/2012/10/17/attenuation-coherent-scatter/

Q36: The two primary forms of x-ray interaction in the diagnostic range are a. Compton scattering and photoelectric absorption. b. Compton scattering and pair production. c. photoelectric absorption and coherent scattering. d. coherent scattering and Thompson scattering. a. Compton scattering and photoelectric absorption.

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Marine Medic

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Marine Medic

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Q37: Coherent scattering Coherent scatter (or Thompson scatter) There are three main steps in coherent scatter.

1. An incoming x ray photon with less than 10 keV (so a very low energy x ray photon) interacts with an outer orbital electron.

2. The incoming x ray photon transfers ALL of its energy to the outer orbital electron. The incoming x ray photon no longer exists after transferring its energy. This makes the outer orbital electron excited.

3. The outer orbital electron gives off the excess energy (in the form of an x ray photon) in a different direction than the original incoming x ray photon. The new x ray photon has the same energy as the incoming x ray photon.

< 10 keV

Charlie Chong/ Fion Zhang

https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q38: What happens to the x-ray in a Photoelectric effect?

It is absorbs and disappears (the excess energy is converted into the kinetic energy of the free electron) Q39: What kvp is used to penetrate barium in a contrast examination?

Approximately 90 kvp

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https://quizlet.com/23654671/x-ray-interactions-flashcards-physics-flash-cards/

Q40: When the kvp is increased, what happens to the absolute probability of the photoelectric effect versus Compton effect?

When kvp is increased the probability of any interaction is reduced but since the probability of PE interaction is reduced much more rapidly that the probability of Compton interaction the relative # of Compton interactions increases

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Q42: Of the five x-ray interactions with matter, three are not important to diagnostic radiology. Which are they and why are they not important?

The x-ray energies of classical scattering, photo disintegration ,pair production are outside the energy range of diagnostic x-ray.

Q42: What are the two factors of importance to differential absorption?

Kev and atomic number of absorber

Q43: A beam containing x-rays or gamma rays that all have the same energy monoenergetic

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Q44: Identify the x-ray interaction with matter Photodisintegration (PD) is the process by which the x-ray photon is captured by the nucleus of the atom with the ejection of a particle from the nucleus when all the energy of the x-ray is given to the nucleus. Because of the enormously high energies involved, this process may be neglected for the energies of x-rays used in radiography.

Q45: A compound used as an aid for imaging internal organs with x-rays Contrast agent Q46: The absorption of an x-ray by ionization.

Photoelectric effect

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Q47: The quantity of matter per unit volume Mass density Q48: Identify pair production.

Photo Q49: Maximum differential absorption is possible with the use of _______kvp. low Q50: As the mass density of the absorber increases what effect does this have on the photoelectric effect?

Proportional increase in PE

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Q51: As the atomic number is increased from Calcium Z #20 to Rhenium Z # 45 what effect does this have on the PE? As atomic number of absorber increase the PE increases Increases proportionately with the cube of the atomic number (PE = KZ3?)

Q52: Increasing the kvp from 50 to 100 has what effect on the PE? As the kvp increases less PE and more Compton Q53: The interaction taking place with inner shell electrons is the__________.

PE- Photoelectric effect

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Q54: What effect does increasing the energy level have on Compton scattering?

Increased scatter relative to PE Increased penetration without interaction Q55: What effect does increasing the mass density of the absorber have on Compton scattering?

A proportional increase in compton scattering Q56: What effect does atomic number of the absorber have on Compton scattering?

No effect on Compton scattering

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Q51: As the atomic number is increased from Calcium Z #20 to Rhenium Z # 45 what effect does this have on the PE? As atomic number of absorber increase the PE increases Increases proportionately with the cube of the atomic number (PE = K¡Z4?)

Q56: What effect does atomic number of the absorber have on Compton scattering? - No effect on Compton scattering

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Q57: Where in the atom does Compton scattering take place?

Outer shell electrons Loosely bound electrons (As opposed to PE, the inner electrons?)

Q58: ____ absorption results in the degree of contrast of an x-ray image Differential absorption Q59: Compton scattering _______ contrast in an x-ray image. reduces Q60: Total x-ray absorption effect Photoelectric effect

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Q61: A PE interaction is more likely to occur with a _____atomic number atoms .

High Example Tungsten-74 Lead- 82 Barium-56 Calcium-20 Iodine-53 Atomic nmber has no effect on compton scattering See Q56: What effect does atomic number of the absorber have on Compton scattering? - No effect on Compton scattering

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Q62: Identify the major source of radiation to the technologist.

The majority of the radiation dose received by the operator is due to scattered radiation from the patient. After interacting with the patient, radiation is scattered more or less uniformly in all directions.

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Q63: Identify the x-ray interaction.

Q64: Compton scattering

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Q65: What are the two electrons created by pair production called?

Negatron & Positron

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Alpha Decay

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https://spec2000.net/06-atomicphysics.htm

Beta Decay N â&#x2020;&#x2019; P + e- + antineutrino

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https://spec2000.net/06-atomicphysics.htm

Beta Decay P â&#x2020;&#x2019; P + e+ + neutrino

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https://spec2000.net/06-atomicphysics.htm

Q65: Pair production requires a photon energy of at least ______ mev.

1.02 mev Q66: An interaction which occurs between low energy x-ray photons and matter Coherent scatter, classical scatter, unmodified scatter, Thomson scatter, Rayleigh scatter.

Q67: When a scattered photon is deflected back toward the source it is called _______ radiation.

Backscatter radiation

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Q68: _______ occurs when an incident x-ray photon interacts with a loosely bound outer shell electron, removes the electron from its shell and then proceeds in a different direction.

Compton scattering Q69: The dislodged electron in a Compton interaction is called a ______.

Compton electron Recoil electron Q70: How is the frequency of the x-ray photon affected by a Compton interaction?

Lower frequency, some energy is lost.

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Q71: What affect does Compton scatter interaction have on the wavelength of the exiting scatter photon?

Wavelength becomes longer, some energy is lost.

Q72: What is the difference between Thomson and Rayleigh scatter radiation?

Both are coherent scatter. Thomson involves a single electron in the interaction while Rayleigh scattering involves all of the electrons of the atom in the interaction.

Q73: Coherent scattering occurs in a very ______ x-ray energy range, which is outside the diagnostic range.

Low energy. Below 10 kev.

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Rayleigh Scattering Rayleigh scattering refers to the scattering of light off of the molecules of the air, and can be extended to scattering from particles up to about a tenth of the wavelength of the light. It is Rayleigh scattering off the molecules of the air which gives us the Blue sky. Lord Rayleigh calculated the scattered intensity from dipole scatterers much smaller than the wavelength to be:

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http://hyperphysics.phy-astr.gsu.edu/hbase/atmos/blusky.html

Rayleigh scattering can be considered to be elastic scattering since the photon energies of the scattered photons is not changed. Scattering in which the scattered photons have either a higher or lower photon energy is called Raman scattering. Usually this kind of scattering involves exciting some vibrational mode of the molecules, giving a lower scattered photon energy, or scattering off an excited vibrational state of a molecule which adds its vibrational energy to the incident photon.

Thomson scattering is the elastic scattering of electromagnetic radiation by a free charged particle, as described by classical electromagnetism. It is just the low-energy limit of Compton scattering: the particle kinetic energy and photon frequency are the same before and after the scattering. This limit is valid as long as the photon energy is much less than the mass energy of the particle: Ѵ ＜＜mc2/h or equivalently, if the wavelength of the light is much greater than the Compton wavelength of the particle. The classical description is also the low-intensity limit

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http://hyperphysics.phy-astr.gsu.edu/hbase/atmos/blusky.html

 Low-energy phenomena: Photoelectric effect  Mid-energy phenomena: Thomson scattering Compton scattering  High-energy phenomena: Pair production Photondisintegration

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https://en.wikipedia.org/wiki/Thomson_scattering

Q74a: What three basic rules which govern the possibility of photoelectric interaction?

1. The incident x-ray photon energy must be greater than the binding energy of the inner shell electron.

2. The PE interaction is more likely to occur when the x-ray photon energy & the electron binding energy are nearer to one another.

3. A PE is more likely to occur with an electron which is more tightly bound.

Q74b: The term used for the reduction in the number of x-ray photons in the beam after it has passed thru matter. attenuation Q75: In pair production to photons are created each with an energy of ____mev.

0.51 mev.

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Q76: True or False: Pair production does not occur in the diagnostic range.

True: Pair production requires 1.02 mev which is much higher energy than the diagnostic range.

Q77: Interactions above 10 Mev are ________ interactions. photodisintegration Q78: Which interaction has a high energy photon strike the nucleus and all of its energy is absorbed by the nucleus causing a nuclear fragment to be emitted? photodisintegration

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Photodisintegration

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Photodisintegration

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Q79: True or False: Pair production does not occur in the diagnostic range.

True: Pair production requires 1.02 mev which is much higher energy than the diagnostic range.

Q80: Interactions above 10 Mev are ________ interactions. photodisintegration Q81: Which interaction has a high energy photon strike the nucleus and all of its energy is absorbed by the nucleus causing a nuclear fragment to be emitted? photodisintegration

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Q82: What affect does a high atomic number have on the binding energy of an element?

Direct relationship. As the number of protons increases with increased atomic number the positive charges increase the binding energy making it more difficult to remove electrons from their shells.

Q83: Which shell will have the highest energy?

The shell furthest from the nucleaus.

Q84: Which shell has the highest binding energy?

Always the K-shell closest to the nucleus.

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Q85: List the 5 basic interactions between x-rays and matter.

1. Photoelectric absorption 2. Coherent scattering 3. Compton scattering 4. Pair production 5. Photodisintegration Q86: Another name for the characteristic photon is ______ radiation.

Secondary.

Q87: What is the primary cause of occupational radiation exposure to radiographers?

Scatter radiation emitted by the patient.

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Q88: ________ interaction the energy of the x-ray photon is converted to matter in the form of two electrons.

Pair production.

Q89: An electron with a positive charge.

Position.

Q90: Which of the five interactions has a significant impact on an x-ray image?

Photoelectric-Compton

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Q91: What affect does increasing the kVp have on PE and Compton scattering?

PE decreases with increasing kVp. Compton increases with increasing kVp requiring the use of a grid to clean up scatter.

Q92: Which interaction is predominant in the human body in the diagnostic xray range?

Compton scattering Q93: When the PE is more prevalent the resulting radiographic image will possess _______ contrast.

High Contrast-Short scale contrast-Very black and white contrast.

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Q94: What affect does increasing the kVp have on PE and Compton scattering?

PE decreases with increasing kVp. Compton increases with increasing kVp requiring the use of a grid to clean up scatter.

Q95: Which interaction is predominant in the human body in the diagnostic xray range?

Compton scattering Q96: When the PE is more prevalent the resulting radiographic image will possess _______ contrast.

High Contrast-Short scale contrast-Very black and white contrast.

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Q97: High contrast images can be created by selecting _______ kVp and ______ mAs. Low kVp and High mAs. Q98: Low contrast images are created by using ______ kVp and ______ mAs. High kVp and Low mAs. Q99: What is backscatter?

When a scattered photon is deflected back toward the source, it is traveling in the opposite direction from the incident photon.

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Q100: Scattering of very low energy x-rays with no loss of energy care called________.

Coherent scattering - Thompson scattering.

(Rayleigh scattering?)

Q101: A generalized dulling of the image by optical densities not representing diagnostic information.

Image fog.

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Q102: The probability of _____ is inversely proportional to the third power of the x-ray energy.

PE, (PE = K¡Z4/ E3?)

Q103: A PE interaction is more likely to occur with a _______ atomic number atoms.

High.

Q51: As the atomic number is increased from Calcium Z #20 to Rhenium Z # 45 what effect does this have on the PE? As atomic number of absorber increase the PE increases Increases proportionately with the cube of the atomic number (PE = K¡Z4?)

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Deep Scratches In Lead Screen For Radiography The number of electrons emitted per unit surface of the lead is essentially uniform. Therefore, more electrons can reach the film in the vicinity of a scratch, resulting in a dark line on the radiograph. (For illustrative clarity, electron paths have been shown as straight and parallel; actually, the electrons are emitted diffusely.)

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In considering the problem of demagnetiz ation, it is important to remember that a part may retain a strong residual field after having been circularly magnetized, and yet exhibit little or no external evidence of such a condition, as local poles are not easily detected. 圆形磁场极点不明显 Such a field is difficult to remove, and there is no easy way to check the success of demagnetization. There may be local poles on a circularly magnetized piece at projecting irregularities or changes or sections, and these can be checked with a field indicator. However, to demagnetize a circularly magnetized part, it is often better to first convert the circular field to a longitudinal field. The longitudinal field does possess external poles, is more easily removed, and the extent of removal can be easily checked with a field indicator.

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http://chemical-biological.tpub.com/TM-1-1500-335-23/css/TM-1-1500-335-23_281.htm

Read More: https://www.nde-ed.org/TeachingResources/teachingresources.htm

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Good Luck!

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