2015 Ph.D. Comprehensive Examination III. Radiological Sciences - Medical Physics

Size: px
Start display at page:

Download "2015 Ph.D. Comprehensive Examination III. Radiological Sciences - Medical Physics"

Transcription

1 January Ph.D. Comprehensive Examination III Radiological Sciences - Medical Physics In this three-hour exam, you are required to answer all of the questions in Part A and any two (2) out of the four (4) problems in Part B. Use one answer book for Part A and one answer book for each of the problems of Part B. Please make sure that your name is on the answer books, that each problem is clearly numbered, and that your final answers (with correct units and number of significant figures) are highlighted by framing or circling. Be certain that you have done all of the short answer questions in Part A, choosing only one answer for each question. Answer no more than two problems from part B (if you offer more than two problems from Part B, only the first two will be graded). Partial credit will be awarded for Part B, but only if you document your work on these two problems in a legible and logical manner (defining variables, declaring assumptions, consolidating units, etc.). The last page contains some useful constants and equations. 1 of 12

2 Part A: Short Answer Questions (Obligatory) 1. Which of the following statements is false regarding exposure and dose to air or soft tissue? a. The mass energy absorption coefficients (μ en /ρ) for air and soft tissue are approximately equal over a broad range of photon energies. b. The definition 1 R / !4 C kg!1 establishes an approximate equality between exposure in the unit of roentgen and dose to soft tissue under the condition of charged particle equilibrium and in units of rad or rem. c. Exposure in the unit of roentgen is a factor of 1.14 greater than the dose to air under the condition of charged particle equilibrium and in the unit of rad. d. The average energy required to produce one coulomb of charge in dry air is 33.7 J. e. Exposure is defined for any form of uncharged ionizing radiation that can produce ion pairs in air Na decays by beta plus decay and emits a positron with a maximum energy of 0.81 MeV and a gamma ray. 22 Na (BE = MeV) decays to 22 Ne (BE = MeV). What is the energy of the gamma ray? a MeV b MeV c MeV d MeV e MeV 3. For equal fluence rates incident on the human body, which of the following radiations will produce the largest dose rate to the skin? a. 2 MeV photons b. 1 MeV beta particles c. 5 MeV alpha particles d. Thermal neutrons e. 40 kev recoil nuclei 2 of 12

3 Part A: Short Answer Questions (Obligatory) 4. Which of the following statements is false regarding the penetration of broad, parallel beams of charged particles in soft tissue? a. Most of the dose for heavy charged particles is delivered near the end of their track. b. A plot of dose vs. depth for heavy charged particles will produce a Bragg Peak. c. The location of a Bragg Peak is useful for planning radiotherapy with proton beams. d. The Bragg peak for heavy charged particles can be broadened by inserting an absorbing material with various thicknesses between the particle beam and the soft tissue. e. A plot of dose vs. depth for electrons in general will be a maximum at the surface and decrease exponentially as depth increases. 5. When MTF of the focal and receptor blur are both equal to 0.1 (at 2 lp/mm), the imaging system MTF at this spatial frequency is most likely: a. 0.2 b. 0.1 c d e The actual anode focal area is 3 mm (length) and 2.5 mm (width) for 16 degree anode angle. The projected focal spot size (mm2) at the central axis is approximately a. 2 b. 3 c. 4 d. 5 e An ultrasound signal attenuated to 1% of its original intensity corresponds to attenuation (-db) of: a. 1 b. 5 c. 10 d. 20 e of 12

4 Part A: Short Answer Questions (Obligatory) 8. The most likely limitation of magnification is an increase in: a. Focal blur b. Scattered photons c. Absorbed photons d. Detector exposure e. Quantum mottle 9. Typical soft tissue differences (%) in spin density are most likely: a. Less than 1 b. 3 c. 10 d. 30 e An ionization chamber designed to satisfy the conditions of Bragg-Gray cavity theory for 662 kev photons contains 6 cm 3 of air at a density of !3 g cm!3. If the current produced by the chamber is 1.4 pa when exposed to a constant fluence rate of 662 kev photons, then what is the exposure rate at the location of the chamber? a. 2.7 R hr!1 b R hr!1 c R hr!1 d R hr!1 e R hr!1 11. A sample containing min 27 Mg with an initial activity of 1 μci was measured for 10 minutes using a detection system with a counting efficiency of 0.3 counts per decay for 27 Mg. What is the expected number of net counts recorded if the 27 Mg sample was measured for 10 minutes? a b c d e of 12

5 Part A: Short Answer Questions (Obligatory) 12. What net counting rate would be observed for a Geiger-Mueller (GM) detector when measuring a 1 mci point source of 137 Cs at 1 m from the detector face? The dead time for this detector is 0.5 ms, and the counting efficiency for this source and geometry and in the absence of dead time losses is !5 counts per decay of 137 Cs. a. 558 cps b. 632 cps c. 925 cps d. 1,033 cps e. 1,720 cps 13. Reference man takes in 3 L/day of water. The total body water in reference man is 42 L. For intakes of tritiated water, reference man is modeled as one compartment with instantaneous and uniform mixing of water intake and excretion. What is the biological half-life of tritiated water in reference man rounded to one significant digit? a days b. 1 day c. 10 days d. 14 days e. 10 years 14. The ratio of the activity of radioactive carbon (C-14, half-life = 5730 years) to stable carbon in living organisms is equal to 16 d/min per gram of carbon. This ratio decreases starting at the time the organism dies. If the ratio in a once living artifact is found to be 2.0 d/min per gram of carbon, how old is the artifact? a years b. 11,500 years c. 11,900 years d. 17,200 years e. 22,900 years 5 of 12

6 Part A: Short Answer Questions (Obligatory) 15. In 10CFR20, a Very High Radiation Area is defined as an area, accesible to individuals, in which radiation levels from radiation sources external to the body could result in an individual receiving an absorbed dose in excess of at a distance of 1 meter in one hour? a. 500 mrads b. 500 rads c. 1 mgy d. 0.5 Gy e. 1 Gy 16. In an experiment with an ion beam, 3 Gy of absorbed dose generates a measurable biological effect. It takes 12 Gy of 250 kvp X-ray radiation to produce the same biological effect. What is the relative biological effectiveness of the ion beam? a. 2.5 b. 3 c. 4 d The Fricke dosimeter provides an example for a. the oxygen effect b. scavenger reactions c. both A and B d. none of the above 18. Which of the following groups of cells are least radiosensitive? a. Adult nerve cells b. Nerve cells in the embryo c. Lymphocytes d. Immature spermatogonia 6 of 12

7 Part A: Short Answer Questions (Obligatory) 19. A tissue with cells of 15 µm in average size and 3.84x10-12 kg in mass is irradiated with 1.0 cgy dose. Assuming that an active event corresponds to 60 ev, the number of events in a cell will be: (a) 1000 (b) 2000 (c) 4000 (d) 8000 (1 J = x ev) 20. With respect to the law of Bergonie and Tribondeau, which of the following sentences would best complete the following statement? "The most pronounced radiation effects occur in cells having the." a. Least reproductive activity, shortest mitotic phases, and most maturity b. Greatest reproductive activity, shortest mitotic phases, and most maturity c. Greatest reproductive activity, longest mitotic phases, and least maturity d. Least reproductive activity, shortest mitotic phases, and least maturity. 7 of 12

8 Problem 1. Ph.D. Comprehensive Examination, January 2015 Part B: Problems (Do any two out of four) An imaged part of a patient's body consists of iodine (thickness x i ), bone (thickness x b ) and soft tissue (thickness x s ). We acquire two exposures at high and low energies, E H and E L, respectively. Derive the formula for the soft tissue cancelled image using the energy subtraction method. Assume that the respective attenuation coefficients for iodine ( i ), bone ( b ), and soft tissue ( s ) are known at both energies. 8 of 12

9 Problem 2. Ph.D. Comprehensive Examination, January 2015 Part B: Problems (Do any two out of four) A beam of 8 MeV electrons with a current equal to 5 milliamperes is incident on a 0.5 mm thick sheet of lead (density = g cm -3 ). The stopping power values for 8 MeV electrons are: Collision (electronic) Mass Stopping Power = (- dt / dx) col = (S / ) col = MeV cm 2 g -1 Radiation (nuclear) Mass Stopping Power = (- dt / dx) rad = (S / ) rad = MeV cm 2 g -1 Total Mass Stopping Power = (- dt / dx) tot = (S / ) tot = MeV cm 2 g -1 Assume that the sheet is thin enough that the stopping power values are constant at all points along the electron s track through the sheet. a. Estimate the energy of the electrons after they penetrate this sheet. Assume that they travel in a straight line perpendicular to the lead sheet. b. Estimate how much bremmstrahlung energy each electron produces. c. What is the average specific ionization for these electrons in this particular sheet of lead if the W value is 25 ev/ion pair? d. What is the fluence rate, in electrons cm -2 sec -1, at the surface of the sheet if the electron beam has a cross sectional area of 5 cm²? e. What is the absorbed dose rate, in rads/h, at the surface of the lead sheet? 9 of 12

10 Problem 3. Ph.D. Comprehensive Examination, January 2015 Part B: Problems (Do any two out of four) Most instruments for detecting radiation involve the ionization of atoms and then the harvesting of that charge, by one means or another, to produce an observable output signal. a. All real detector materials have many ways of absorbing energy, and only some are ionizing. Thus, the concept of an "effective" ionization potential, W, which is bigger than the true ionization potential, usually about double. If for some material, and some radiation, W = 20 ev, how many charge carriers, N, would radiation of 1 MeV cause? b. If N followed Poisson statistics, and remembering the variance, 2 = N, what would you expect the energy resolution of such a detector to be? c. In real life, for real materials, the correlations between ionizing and non-ionizing processes mean the energy resolution is better than the expectation from a Poisson distribution and 2 = F N with 0 < F < 1. What is this factor, F? Is F = 1 better than F = 0? d. For semiconductor detectors like silicon and germanium spectrometers (which for most radiation detectors is the optimum material for energy resolution) name TWO reasons why the energy resolution is far superior to most other materials. 10 of 12

11 Problem 4. Ph.D. Comprehensive Examination, January 2015 Part B: Problems (Do any two out of four) In an experiment using HeLa cells under oxygenated and anoxic conditions, the following survival curve was determined. The LQ model was found a good fit to these survival curves with the following parameters: For the oxygenated case, = 3.0E-1 and = 7.0E-2. For the anoxic case, = 1.0E-1 and = 4.0E-2. a. Determine the oxygen enhancement ratio at SF=0.1 and at SF=0.01. b. For each case, determine the dose where the linear contribution to cell killing equals the quadratic contribution. c. What oxygen enhancement ratio would you anticipate at SF=0.001 based on the above data? Justify your answer. 11 of 12

12 Part B: Problems (Do any two out of four) Useful Constants and Equations X = (μ en /ρ) air Φ T (e/w) D cpe = (μ en /ρ) Φ T K = (μ tr /ρ) Φ T D = (S col /ρ) Φ X = A Γ / r² X = 6 C E D = 300 A H = D Q X disc = π A a Γ ln[1 + (R/x)² ] X line = (A l Γ/x) tan -1 (L/x) = (A l Γ/x) Σ = σ ρ atom ρ atom = ρ N A / W R = Σ Φ = μ Φ Φ = S / 4 π r² Ω = A / R² Ω = 2 π (1 - x / R ) f = Ω / 4 Q = T = BE + Q nt = - m 0 c 2 N(t) = (P t) [ (1 - e -k t ) / k t ] P = U R F / λ P = σ Φ 0 N target A = λ N C = E D R = E A S = A Y D(T) = N (1 - e -λt ) e -x = 1 - x + x 2 /2! - x 3 /3! +... A air = A tissue = 12.8 A water = 13.4 W = 33.7 ev/ion pair e = 1.602x10-19 C N A = 6.022x10 23 c 2 = Mev/amu R = 2.58x10-4 C/kg Gy = 100 rad = 1 J/kg rad = 6.242x10 7 MeV/g amp = C/s ev = 1.602x10-19 J Ci = 3.7x10 10 Bq = 3.7x10 10 d/s barn = cm 2 watt = J/s 12 of 12

Gy can be used for any type of radiation. Gy does not describe the biological effects of the different radiations.

Gy can be used for any type of radiation. Gy does not describe the biological effects of the different radiations. Absorbed Dose Dose is a measure of the amount of energy from an ionizing radiation deposited in a mass of some material. SI unit used to measure absorbed dose is the gray (Gy). 1J 1 Gy kg Gy can be used

More information

11/23/2014 RADIATION AND DOSE MEASUREMENTS. Units of Radioactivity

11/23/2014 RADIATION AND DOSE MEASUREMENTS. Units of Radioactivity CHAPTER 4 RADIATION UNITS RADIATION AND DOSE MEASUREMENTS 1 Units of Radioactivity 2 1 Radiation Units There are specific units for the amount of radiation you receive in a given time and for the total

More information

Radiation Quantities and Units

Radiation Quantities and Units Radiation Quantities and Units George Starkschall, Ph.D. Lecture Objectives Define and identify units for the following: Exposure Kerma Absorbed dose Dose equivalent Relative biological effectiveness Activity

More information

Outline. Radiation Interactions. Spurs, Blobs and Short Tracks. Introduction. Radiation Interactions 1

Outline. Radiation Interactions. Spurs, Blobs and Short Tracks. Introduction. Radiation Interactions 1 Outline Radiation Interactions Introduction Interaction of Heavy Charged Particles Interaction of Fast Electrons Interaction of Gamma Rays Interactions of Neutrons Radiation Exposure & Dose Sources of

More information

Unit 08 Nuclear Structure. Unit 08 Nuclear Structure Slide 1

Unit 08 Nuclear Structure. Unit 08 Nuclear Structure Slide 1 Unit 08 Nuclear Structure Unit 08 Nuclear Structure Slide 1 The Plan Nuclear Structure Nuclear Decays Measuring Radiation Nuclear Power Plants Major Nuclear Power Accidents New Possibilities for Nuclear

More information

4.1b - Cavity Theory Lecture 2 Peter R Al mond 2011 Overview of Lecture Exposure (W/e)air Exposure Exposure and and and Air Air Kerma

4.1b - Cavity Theory Lecture 2 Peter R Al mond 2011 Overview of Lecture Exposure (W/e)air Exposure Exposure and and and Air Air Kerma 4.1b - Cavity Theory Lecture 2 Peter R Almond 2011 Overview of Lecture Exposure (W/e) air Exposure and Air Kerma Exposure Exposure is symbolized as X and defined by the ICRU as the quotient of dq by dm,

More information

Radiation and Radioactivity. PHYS 0219 Radiation and Radioactivity

Radiation and Radioactivity. PHYS 0219 Radiation and Radioactivity Radiation and Radioactivity 1 Radiation and Radioactivity This experiment has four parts: 1. Counting Statistics 2. Gamma (g) Ray Absorption Half-length and shielding 3. 137 Ba Decay Half-life 4. Dosimetry

More information

INTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017

INTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017 INTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017 This is a closed book examination. Adequate information is provided you to solve all problems. Be sure to show all work, as partial credit

More information

Physics 219 Help Session. Date: Wed 12/07, Time: 6:00-8:00 pm. Location: Physics 331

Physics 219 Help Session. Date: Wed 12/07, Time: 6:00-8:00 pm. Location: Physics 331 Lecture 25-1 Physics 219 Help Session Date: Wed 12/07, 2016. Time: 6:00-8:00 pm Location: Physics 331 Lecture 25-2 Final Exam Dec. 14. 2016. 1:00-3:00pm in Phys. 112 Bring your ID card, your calculator

More information

LET! (de / dx) 1 Gy= 1 J/kG 1Gy=100 rad. m(kg) dose rate

LET! (de / dx) 1 Gy= 1 J/kG 1Gy=100 rad. m(kg) dose rate Basics of Radiation Dosimetry for the Physicist http://en.wikipedia.org/wiki/ionizing_radiation I. Ionizing radiation consists of subatomic particles or electromagnetic waves that ionize electrons along

More information

APPENDIX A RADIATION OVERVIEW

APPENDIX A RADIATION OVERVIEW Former NAVWPNSTA Concord, Inland Area APPENDIX A RADIATION OVERVIEW Draft ECSD-3211-0005-0004 08/2009 This page intentionally left blank. Draft ECSD-3211-0005-0004 08/2009 APPENDIX A RADIATION OVERVIEW

More information

CHARGED PARTICLE INTERACTIONS

CHARGED PARTICLE INTERACTIONS CHARGED PARTICLE INTERACTIONS Background Charged Particles Heavy charged particles Charged particles with Mass > m e α, proton, deuteron, heavy ion (e.g., C +, Fe + ), fission fragment, muon, etc. α is

More information

05/11/2013. Nuclear Fuel Cycle Ionizing radiation. Typical decay energies. Radiation with energy > 100 ev. Ionize an atom < 15eV

05/11/2013. Nuclear Fuel Cycle Ionizing radiation. Typical decay energies. Radiation with energy > 100 ev. Ionize an atom < 15eV Nuclear Fuel Cycle 2013 Lecture 4: Interaction of Ionizing Radiation with Matter Ionizing radiation Radiation with energy > 100 ev Ionize an atom < 15eV Break a bond 1-5 ev Typical decay energies α: 4-9

More information

Nuclear Spectroscopy: Radioactivity and Half Life

Nuclear Spectroscopy: Radioactivity and Half Life Particle and Spectroscopy: and Half Life 02/08/2018 My Office Hours: Thursday 1:00-3:00 PM 212 Keen Building Outline 1 2 3 4 5 Some nuclei are unstable and decay spontaneously into two or more particles.

More information

Lab #13: MEASUREMENT OF RADIATION DOSES

Lab #13: MEASUREMENT OF RADIATION DOSES Lab #13: MEASUREMENT OF RADIATION DOSES THEORETICAL BACKGROUND In order to estimate the radiation exposure it is essential to determine the quantity of radiation. If we identify the dose of radiation to

More information

Some nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle

Some nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle Radioactivity George Starkschall, Ph.D. Lecture Objectives Identify methods for making radioactive isotopes Recognize the various types of radioactive decay Interpret an energy level diagram for radioactive

More information

PS-21 First Spring Institute say : Teaching Physical Science. Radioactivity

PS-21 First Spring Institute say : Teaching Physical Science. Radioactivity PS-21 First Spring Institute say 2012-2013: Teaching Physical Science Radioactivity What Is Radioactivity? Radioactivity is the release of tiny, highenergy particles or gamma rays from the nucleus of an

More information

GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY

GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY ABSORBED DOSE: The amount of energy absorbed, as a result of radiation passing through a material, per unit mass of material. Measured in rads (1 rad

More information

Radiation Protection & Radiation Therapy

Radiation Protection & Radiation Therapy Radiation Protection & Radiation Therapy For Medical Students Professor of Medical Physics Radiation Units Activity Number disintegrations per second (Curie, Becquerel) Exposure (Roentgen, C/kg) Absorbed

More information

Georgia Institute of Technology. Radiation Detection & Protection (Day 3)

Georgia Institute of Technology. Radiation Detection & Protection (Day 3) Georgia Institute of Technology The George W. Woodruff School of Mechanical Engineering Nuclear & Radiological Engineering/Medical Physics Program Ph.D. Qualifier Exam Spring Semester 2009 Your ID Code

More information

Radiation Dose, Biology & Risk

Radiation Dose, Biology & Risk ENGG 167 MEDICAL IMAGING Lecture 2: Sept. 27 Radiation Dosimetry & Risk References: The Essential Physics of Medical Imaging, Bushberg et al, 2 nd ed. Radiation Detection and Measurement, Knoll, 2 nd Ed.

More information

Chapter V: Cavity theories

Chapter V: Cavity theories Chapter V: Cavity theories 1 Introduction Goal of radiation dosimetry: measure of the dose absorbed inside a medium (often assimilated to water in calculations) A detector (dosimeter) never measures directly

More information

INTRODUCTION TO IONIZING RADIATION (Attix Chapter 1 p. 1-5)

INTRODUCTION TO IONIZING RADIATION (Attix Chapter 1 p. 1-5) INTRODUCTION TO IONIZING RADIATION (Attix Chapter 1 p. 1-5) Ionizing radiation: Particle or electromagnetic radiation that is capable of ionizing matter. IR interacts through different types of collision

More information

Basic physics Questions

Basic physics Questions Chapter1 Basic physics Questions S. Ilyas 1. Which of the following statements regarding protons are correct? a. They have a negative charge b. They are equal to the number of electrons in a non-ionized

More information

Ch. 18 Problems, Selected solutions. Sections 18.1

Ch. 18 Problems, Selected solutions. Sections 18.1 Sections 8. 8. (I) How many ion pairs are created in a Geiger counter by a 5.4-MeV alpha particle if 80% of its energy goes to create ion pairs and 30 ev (average in gases) is required per ion pair? Notice

More information

PHY138Y Nuclear and Radiation

PHY138Y Nuclear and Radiation PHY138Y Nuclear and Radiation Professor Tony Key MP401 key@physics.utoronto.ca Announcements Next and last Representative Assembly, Friday of next week (23 rd ) MP713 me 12:10 FRIDAY 23 rd FREE COOKIES

More information

Dosimetry. Sanja Dolanski Babić May, 2018.

Dosimetry. Sanja Dolanski Babić May, 2018. Dosimetry Sanja Dolanski Babić May, 2018. What s the difference between radiation and radioactivity? Radiation - the process of emitting energy as waves or particles, and the radiated energy Radioactivity

More information

Number of protons. 2. What is the nuclear symbol for a radioactive isotope of copper with a mass number of 60? A) Cu

Number of protons. 2. What is the nuclear symbol for a radioactive isotope of copper with a mass number of 60? A) Cu Chapter 5 Nuclear Chemistry Practice Problems 1. Fill in the missing information in the chart: Medical Use Atomic Mass symbol number Heart imaging 201 Tl 81 Number of protons Number of neutrons Abdominal

More information

11 Gamma Ray Energy and Absorption

11 Gamma Ray Energy and Absorption 11 Gamma Ray Energy and Absorption Before starting this laboratory, we must review the physiological effects and the proper use of the radioactive samples you will be using during the experiment. Physiological

More information

Radioactive nuclei. From Last Time. Biological effects of radiation. Radioactive decay. A random process. Radioactive tracers. e r t.

Radioactive nuclei. From Last Time. Biological effects of radiation. Radioactive decay. A random process. Radioactive tracers. e r t. From Last Time Nuclear structure and isotopes Binding energy of nuclei Radioactive nuclei Final Exam is Mon Dec 21, 5:05 pm - 7:05 pm 2103 Chamberlin 3 equation sheets allowed About 30% on new material

More information

Properties of the nucleus. 8.2 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus

Properties of the nucleus. 8.2 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus Properties of the nucleus 8. Nuclear Physics Properties of nuclei Binding Energy Radioactive decay Natural radioactivity Consists of protons and neutrons Z = no. of protons (Atomic number) N = no. of neutrons

More information

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na Ellen Simmons 1 Contents Introduction Review of the Types of Radiation Charged Particle Radiation Detection Review of Semiconductor

More information

9 Nuclear decay Answers to exam practice questions

9 Nuclear decay Answers to exam practice questions Pages 173 178 Exam practice questions 1 X-rays are quanta of energy emitted when electrons fall to a lower energy level, and so do not emanate from the nucleus Answer D. 2 Alpha particles, being the most

More information

Rad T 290 Worksheet 2

Rad T 290 Worksheet 2 Class: Date: Rad T 290 Worksheet 2 1. Projectile electrons travel from a. anode to cathode. c. target to patient. b. cathode to anode. d. inner shell to outer shell. 2. At the target, the projectile electrons

More information

Shielding of Ionising Radiation with the Dosimetry & Shielding Module

Shielding of Ionising Radiation with the Dosimetry & Shielding Module Shielding of Ionising Radiation with the Dosimetry & Shielding Module J. Magill Overview Biological Effects of Ionising Radiation - Absorber dose, Quality or Weighting Factor, Equivalent Dose Attenuation

More information

Today, I will present the first of two lectures on neutron interactions.

Today, I will present the first of two lectures on neutron interactions. Today, I will present the first of two lectures on neutron interactions. I first need to acknowledge that these two lectures were based on lectures presented previously in Med Phys I by Dr Howell. 1 Before

More information

Outline. Absorbed Dose in Radioactive Media. Introduction. Radiation equilibrium. Charged-particle equilibrium

Outline. Absorbed Dose in Radioactive Media. Introduction. Radiation equilibrium. Charged-particle equilibrium Absorbed Dose in Radioactive Media Chapter F.A. Attix, Introduction to Radiological Physics and Radiation Dosimetry Outline General dose calculation considerations, absorbed fraction Radioactive disintegration

More information

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther

More information

Chapter 29. Nuclear Physics

Chapter 29. Nuclear Physics Chapter 29 Nuclear Physics Ernest Rutherford 1871 1937 Discovery that atoms could be broken apart Studied radioactivity Nobel prize in 1908 Some Properties of Nuclei All nuclei are composed of protons

More information

Atoms, Radiation, and Radiation Protection

Atoms, Radiation, and Radiation Protection James E. Turner Atoms, Radiation, and Radiation Protection Third, Completely Revised and Enlarged Edition BICENTENNIAL J 0 1 8 0 Q 71 z m z CAVILEY 2007 1 ;Z z ü ; m r B10ENTENNIAL WILEY-VCH Verlag GmbH

More information

Chapiter VII: Ionization chamber

Chapiter VII: Ionization chamber Chapiter VII: Ionization chamber 1 Types of ionization chambers Sensitive volume: gas (most often air direct measurement of exposure) ionization chamber Sensitive volume: semiconductor (silicon, germanium,

More information

Interaction of Particles and Matter

Interaction of Particles and Matter MORE CHAPTER 11, #7 Interaction of Particles and Matter In this More section we will discuss briefly the main interactions of charged particles, neutrons, and photons with matter. Understanding these interactions

More information

ZX or X-A where X is chemical symbol of element. common unit: [unified mass unit = u] also known as [atomic mass unit = amu] or [Dalton = Da]

ZX or X-A where X is chemical symbol of element. common unit: [unified mass unit = u] also known as [atomic mass unit = amu] or [Dalton = Da] 1 Part 5: Nuclear Physics 5.1. The Nucleus = atomic number = number of protons N = neutron number = number of neutrons = mass number = + N Representations: X or X- where X is chemical symbol of element

More information

Properties of the nucleus. 9.1 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus

Properties of the nucleus. 9.1 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus Properties of the nucleus 9. Nuclear Physics Properties of nuclei Binding Energy Radioactive decay Natural radioactivity Consists of protons and neutrons Z = no. of protons (tomic number) N = no. of neutrons

More information

College Physics B - PHY2054C

College Physics B - PHY2054C College - PHY2054C Physics - Radioactivity 11/24/2014 My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building Review Question 1 Isotopes of an element A have the same number of protons and electrons,

More information

Radiation Detection and Measurement

Radiation Detection and Measurement Radiation Detection and Measurement June 2008 Tom Lewellen Tkldog@u.washington.edu Types of radiation relevant to Nuclear Medicine Particle Symbol Mass (MeV/c 2 ) Charge Electron e-,! - 0.511-1 Positron

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 19 Modern Physics Nuclear Physics Nuclear Reactions Medical Applications Radiation Detectors Chapter 29 http://www.physics.wayne.edu/~alan/2140website/main.htm 1 Lightning

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lightning Review Lecture 19 Modern Physics Nuclear Physics Nuclear Reactions Medical Applications Radiation Detectors Chapter 29 http://www.physics.wayne.edu/~alan/2140website/main.htm

More information

Technical University of Denmark

Technical University of Denmark Technical University of Denmark Page 1 of 10 pages Written test, 12 December 2012 Course name: Introduction to medical imaging Course no. 31540 Aids allowed: None. Pocket calculator not allowed "Weighting":

More information

Radiological Preparedness & Emergency Response. Session II. Objectives. Basic Radiation Physics

Radiological Preparedness & Emergency Response. Session II. Objectives. Basic Radiation Physics Radiological Preparedness & Emergency Response Session II Basic Radiation Physics Objectives Discuss the difference between ionizing and non-ionizing radiation. Describe radioactive decay. Discuss the

More information

NE 495 Elements of Nuclear Engineering

NE 495 Elements of Nuclear Engineering Name: NE 495 Elements of Nuclear Engineering Open Books and Notes Final Examination, Spring 2009 1. Indicate whether the following statements are true (T) or false (F). [50 ( ) The energy of a photon is

More information

INAYA MEDICAL COLLEGE (IMC) RAD LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM

INAYA MEDICAL COLLEGE (IMC) RAD LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM INAYA MEDICAL COLLEGE (IMC) RAD 232 - LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM Radiation: It is defined as the process by which energy is emitted from a source and propagated through the surrounding

More information

Overview: In this experiment we will study the decay of a radioactive nucleus, Cesium. Figure 1: The Decay Modes of Cesium 137

Overview: In this experiment we will study the decay of a radioactive nucleus, Cesium. Figure 1: The Decay Modes of Cesium 137 Radioactivity (Part I and Part II) Objectives: To measure the absorption of beta and gamma rays To understand the concept of half life and to measure the half life of Ba 137* Apparatus: Radioactive source,

More information

Interaction of Ionizing Radiation with Matter

Interaction of Ionizing Radiation with Matter Interaction of Ionizing Radiation with Matter Interaction of neutrons with matter Neutral particles, no repulsion with the positively charged nucleus: important projectile Origin of the neutrons: Nuclear

More information

CHARGED PARTICLE IONIZATION AND RANGE

CHARGED PARTICLE IONIZATION AND RANGE CHAGD PATICL IONIZATION AND ANG Unlike the neutral radiations (e.g., neutrons and gamma/x rays), the charged particles (e.g., electrons, protons and alphas) are subjected to the coulombic forces from electrons

More information

INAYA MEDICAL COLLEGE (IMC) RAD LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM

INAYA MEDICAL COLLEGE (IMC) RAD LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM INAYA MEDICAL COLLEGE (IMC) RAD 232 - LECTURE 1 RADIATION PHYSICS DR. MOHAMMED MOSTAFA EMAM LECTURES & CLASS ACTIVITIES https://inayacollegedrmohammedemam.wordpress.com/ Password: drmohammedemam 16-02-2015

More information

APPLIED RADIATION PHYSICS

APPLIED RADIATION PHYSICS A PRIMER IN APPLIED RADIATION PHYSICS F A SMITH Queen Mary & Westfield College, London fe World Scientific m Singapore * New Jersey London Hong Kong CONTENTS CHAPTER 1 : SOURCES of RADIATION 1.1 Introduction

More information

Physics of Particle Beams. Hsiao-Ming Lu, Ph.D., Jay Flanz, Ph.D., Harald Paganetti, Ph.D. Massachusetts General Hospital Harvard Medical School

Physics of Particle Beams. Hsiao-Ming Lu, Ph.D., Jay Flanz, Ph.D., Harald Paganetti, Ph.D. Massachusetts General Hospital Harvard Medical School Physics of Particle Beams Hsiao-Ming Lu, Ph.D., Jay Flanz, Ph.D., Harald Paganetti, Ph.D. Massachusetts General Hospital Harvard Medical School PTCOG 53 Education Session, Shanghai, 2014 Dose External

More information

Radiation Safety Talk. UC Santa Cruz Physics 133 Winter 2018

Radiation Safety Talk. UC Santa Cruz Physics 133 Winter 2018 Radiation Safety Talk UC Santa Cruz Physics 133 Winter 2018 Outline Types of radiation Sources of radiation Dose limits and risks ALARA principle Safety procedures Types of radiation Radiation is energy

More information

Nicholas J. Giordano. Chapter 30. Nuclear Physics. Marilyn Akins, PhD Broome Community College

Nicholas J. Giordano.   Chapter 30. Nuclear Physics. Marilyn Akins, PhD Broome Community College Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 30 Nuclear Physics Marilyn Akins, PhD Broome Community College Atomic Nuclei Rutherford s discovery of the atomic nucleus caused scientists

More information

11/19/2014. Chapter 3: Interaction of Radiation with Matter in Radiology and Nuclear Medicine. Nuclide Families. Family Nuclides with Same: Example

11/19/2014. Chapter 3: Interaction of Radiation with Matter in Radiology and Nuclear Medicine. Nuclide Families. Family Nuclides with Same: Example 2014-2015 Residents' Core Physics Lectures Mondays 7:00-8:00 am in VA Radiology and UCSDMC Lasser Conference Rooms Topic Chapters Date Faculty 1 Introduction and Basic Physics 1, 2 M 11/17 Andre 2 Interaction

More information

Unit 6 Modern Physics

Unit 6 Modern Physics Unit 6 Modern Physics Early Booklet E.C.: + 1 Unit 6 Hwk. Pts.: / 46 Unit 6 Lab Pts.: / 16 Late, Incomplete, No Work, No Units Fees? Y / N Essential Fundamentals of Modern Physics 1. A photon s energy

More information

Final Exam. Evaluations. From last time: Alpha radiation. Beta decay. Decay sequence of 238 U

Final Exam. Evaluations. From last time: Alpha radiation. Beta decay. Decay sequence of 238 U Evaluations Please fill out evaluation and turn it in. Written comments are very helpful! Lecture will start 12:15 Today, evaluate Prof. Rzchowski If you weren t here Tuesday, also evaluate Prof. Montaruli

More information

Neutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321

Neutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321 Neutron Interactions Part I Rebecca M. Howell, Ph.D. Radiation Physics rhowell@mdanderson.org Y2.5321 Why do we as Medical Physicists care about neutrons? Neutrons in Radiation Therapy Neutron Therapy

More information

WHAT IS IONIZING RADIATION

WHAT IS IONIZING RADIATION WHAT IS IONIZING RADIATION Margarita Saraví National Atomic Energy Commission - Argentina Workshop on Ionizing Radiation SIM Buenos Aires 10 November 2011 What is ionizing radiation? What is ionizing radiation?

More information

Chapter 42. Nuclear Physics

Chapter 42. Nuclear Physics Chapter 42 Nuclear Physics In the previous chapters we have looked at the quantum behavior of electrons in various potentials (quantum wells, atoms, etc) but have neglected what happens at the center of

More information

III. Energy Deposition in the Detector and Spectrum Formation

III. Energy Deposition in the Detector and Spectrum Formation 1 III. Energy Deposition in the Detector and Spectrum Formation a) charged particles Bethe-Bloch formula de 4πq 4 z2 e 2m v = NZ ( ) dx m v ln ln 1 0 2 β β I 0 2 2 2 z, v: atomic number and velocity of

More information

Interactions with Matter Photons, Electrons and Neutrons

Interactions with Matter Photons, Electrons and Neutrons Interactions with Matter Photons, Electrons and Neutrons Ionizing Interactions Jason Matney, MS, PhD Interactions of Ionizing Radiation 1. Photon Interactions Indirectly Ionizing 2. Charge Particle Interactions

More information

Physics of particles. H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School

Physics of particles. H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School Physics of particles H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School Introduction Dose The ideal dose distribution ideal Dose: Energy deposited Energy/Mass Depth [J/kg] [Gy] Introduction

More information

INTERACTIONS OF RADIATION WITH MATTER

INTERACTIONS OF RADIATION WITH MATTER INTERACTIONS OF RADIATION WITH MATTER Renée Dickinson, MS, DABR Medical Physicist University of Washington Medical Center Department of Radiology Diagnostic Physics Section Outline Describe the various

More information

Classroom notes for: Radiation and Life Lecture Thomas M. Regan Pinanski 207 ext 3283

Classroom notes for: Radiation and Life Lecture Thomas M. Regan Pinanski 207 ext 3283 Classroom notes for: Radiation and Life Lecture 11 98.101.201 Thomas M. Regan Pinanski 207 ext 3283 1 Radioactive Decay Series ( Chains ) A radioactive isotope (radioisotope) can decay and transform into

More information

Nuclear Fusion and Radiation

Nuclear Fusion and Radiation Nuclear Fusion and Radiation Lecture 9 (Meetings 23 & 24) Eugenio Schuster schuster@lehigh.edu Mechanical Engineering and Mechanics Lehigh University Nuclear Fusion and Radiation p. 1/42 Radiation Interactions

More information

Interactions of Radiation with Matter

Interactions of Radiation with Matter Main points from last week's lecture: Decay of Radioactivity Mathematics description nly yields probabilities and averages Interactions of Radiation with Matter William Hunter, PhD" Decay equation: N(t)

More information

Industrial Hygiene: Assessment and Control of the Occupational Environment

Industrial Hygiene: Assessment and Control of the Occupational Environment Industrial Hygiene: Assessment and Control of the Occupational Environment Main Topics Air Pollution Control Analytical Methods Ergonomics Gas and Vapour Sampling General Practice Heat and Cold Stress

More information

Question. 1. Which natural source of background radiation do you consider as dominant?

Question. 1. Which natural source of background radiation do you consider as dominant? Question 1. Which natural source of background radiation do you consider as dominant? 2. Is the radiation background constant or does it change with time and location? 3. What is the level of anthropogenic

More information

Ionization Chamber. Pocket dosimeter

Ionization Chamber. Pocket dosimeter Ionization Chamber Pocket dosimeter 1 Ionization Chamber Pocket dosimeter 2 Radiation Quantities and Units Radiation measurements require specification of the radiation field at various points At the source

More information

Chapter Four (Interaction of Radiation with Matter)

Chapter Four (Interaction of Radiation with Matter) Al-Mustansiriyah University College of Science Physics Department Fourth Grade Nuclear Physics Dr. Ali A. Ridha Chapter Four (Interaction of Radiation with Matter) Different types of radiation interact

More information

Principles of applied dosimetry - illustrated by ionometry. Lesson FYSKJM4710 Eirik Malinen

Principles of applied dosimetry - illustrated by ionometry. Lesson FYSKJM4710 Eirik Malinen Principles of applied dosimetry - illustrated by ionometry Lesson FYSKJM4710 Eirik Malinen Ionometry Ionometry: the art of measuring ionizations Number of ionizations proportional to dose Air filled ionization

More information

Chapter 10 - Nuclear Physics

Chapter 10 - Nuclear Physics The release of atomic energy has not created a new problem. It has merely made more urgent the necessity of solving an existing one. -Albert Einstein David J. Starling Penn State Hazleton PHYS 214 Ernest

More information

Overview: In this experiment we study the decay of a radioactive nucleus, Cesium 137. Figure 1: The Decay Modes of Cesium 137

Overview: In this experiment we study the decay of a radioactive nucleus, Cesium 137. Figure 1: The Decay Modes of Cesium 137 Radioactivity (Part I and Part II) 7-MAC Objectives: To measure the absorption of beta and gamma rays To understand the concept of half life and to measure the half life of Ba 137* Apparatus: Radioactive

More information

Nuclear forces and Radioactivity. Two forces are at work inside the nucleus of an atom

Nuclear forces and Radioactivity. Two forces are at work inside the nucleus of an atom Nuclear forces and Radioactivity Two forces are at work inside the nucleus of an atom Forces act in opposing directions Electrostatic repulsion: pushes protons apart Strong nuclear force: pulls protons

More information

sample What happens when we are exposed to radiation? 1.1 Natural radiation Cosmic radiation

sample What happens when we are exposed to radiation? 1.1 Natural radiation Cosmic radiation 1.1 Natural radiation 3 1 What happens when we are exposed to radiation? 1.1 Natural radiation For as long as humans have walked the earth, we have continually been exposed to naturally-occurring radiation.

More information

Initial Certification

Initial Certification Initial Certification Medical Physics Part 1 Content Guide Part 1 Content Guides and Sample Questions PLEASE NOTE: List of Constants and Physical Values for Use on the Part 1 Physics Exam The ABR provides

More information

Radiation Safety Training Session 1: Radiation Protection Fundamentals and Biological Effects

Radiation Safety Training Session 1: Radiation Protection Fundamentals and Biological Effects Radiation Safety Training Session 1: Radiation Protection Fundamentals and Biological Effects Reading Assignment: LLE Radiological Controls Manual (LLEINST 6610) Part 1 UR Radiation Safety Training Manual

More information

Nuclear Radiation. Natural Radioactivity. A person working with radioisotopes wears protective clothing and gloves and stands behind a shield.

Nuclear Radiation. Natural Radioactivity. A person working with radioisotopes wears protective clothing and gloves and stands behind a shield. Nuclear Radiation Natural Radioactivity A person working with radioisotopes wears protective clothing and gloves and stands behind a shield. 1 Radioactive Isotopes A radioactive isotope has an unstable

More information

Introduction to Medical Imaging Chapter 1 Radiation and the Atom Chapter 2 Interaction of Radiation and Matter Chapter 3

Introduction to Medical Imaging Chapter 1 Radiation and the Atom Chapter 2 Interaction of Radiation and Matter Chapter 3 Introduction to Medical Imaging Chapter 1 Radiation and the Atom Chapter 2 Interaction of Radiation and Matter Chapter 3 Professor, Radiology and Medical Education Director, Diagnostic Physics a copy of

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS OPTION I-2 MEDICAL IMAGING Reading Activity Answers IB Assessment Statements Option I-2, Medical Imaging: X-Rays I.2.1. I.2.2. I.2.3. Define

More information

Study Guide 7: Ionizing Radiation

Study Guide 7: Ionizing Radiation Study Guide 7: Ionizing Radiation Text: Chapter 6, sections 1-11 (more than described in Study Guide), plus text 2.5 and lab manual section 7A-1 (on inverse-square law). Upcoming quizzes: Quiz 4 (final

More information

Radiation Protection Fundamentals and Biological Effects: Session 1

Radiation Protection Fundamentals and Biological Effects: Session 1 Radiation Protection Fundamentals and Biological Effects: Session 1 Reading assignment: LLE Radiological Controls Manual (LLEINST 6610): Part 1 UR Radiation Safety Training Manual and Resource Book: Parts

More information

Physics of Radiography

Physics of Radiography EL-GY 6813 / BE-GY 6203 / G16.4426 Medical Imaging Physics of Radiography Jonathan Mamou and Yao Wang Polytechnic School of Engineering New York University, Brooklyn, NY 11201 Based on Prince and Links,

More information

Radiation Fundamentals. Radiation Safety Training Module 1

Radiation Fundamentals. Radiation Safety Training Module 1 Radiation Fundamentals Module 1 Radioactivity Radioactivity is the process of unstable (or radioactive) atoms becoming stable. This is done by emitting radiation. This process over a period of time is

More information

EEE4106Z Radiation Interactions & Detection

EEE4106Z Radiation Interactions & Detection EEE4106Z Radiation Interactions & Detection 2. Radiation Detection Dr. Steve Peterson 5.14 RW James Department of Physics University of Cape Town steve.peterson@uct.ac.za May 06, 2015 EEE4106Z :: Radiation

More information

General Overview of Gas Filled Detectors

General Overview of Gas Filled Detectors GAS-FILLED DETECTOR General Overview of Gas Filled Detectors Gas-Filled Detectors Ion chamber Proportional counter G-M (Geiger-Miller) counter Diagram of a Generic Gas-Filled Detector A Anode High-voltage

More information

y loo Physics Essentials Workbook Stage 2 Physics Exercises

y loo Physics Essentials Workbook Stage 2 Physics Exercises 238 Physics Essentials Workbook Stage 2 Physics 15.1 2 Exercises P Explain why stable nuclei of high mass have a higher proportion of neutrons than stable nuclei of low mass. 2 Name four types of spontaneous

More information

Queen s University PHYS 352

Queen s University PHYS 352 Page 1 of 5 Queen s University Faculty of Applied Science; Faculty of Arts and Science Department of Physics, Engineering Physics and Astronomy PHYS 352 Measurement, Instrumentation and Experiment Design

More information

Radioactivity. Lecture 7 Dosimetry and Exposure Limits

Radioactivity. Lecture 7 Dosimetry and Exposure Limits Radioactivity Lecture 7 Dosimetry and Exposure Limits Radiation Exposure - Radiology The radiation impact on biological and genetic materials requires some protective measures! Units for scaling the decay

More information

Radiation Physics PHYS /251. Prof. Gocha Khelashvili

Radiation Physics PHYS /251. Prof. Gocha Khelashvili Radiation Physics PHYS 571-051/251 Prof. Gocha Khelashvili Interaction of Radiation with Matter: Heavy Charged Particles Directly and Indirectly Ionizing Radiation Classification of Indirectly Ionizing

More information

Glossary of Terms* BIOASSAY: Assay and measurement procedures used to determine the amount of radioactive material in a biological system.

Glossary of Terms* BIOASSAY: Assay and measurement procedures used to determine the amount of radioactive material in a biological system. Glossary of Terms* *With permission from the Manual of Policies and Procedures for Radiation Protection, for the University of Minnesota, Department of Environmental Health and Safety, Radiation Protection

More information

Image quality assessment. Question: which is a better image? Answer: what are you trying to do?

Image quality assessment. Question: which is a better image? Answer: what are you trying to do? Image Quality Image quality assessment Question: which is a better image? Answer: what are you trying to do? Image Quality Image quality, for the purposes of medical imaging, can be defined as the ability

More information

Georgia Institute of Technology. Radiation Physics (Day 1)

Georgia Institute of Technology. Radiation Physics (Day 1) Georgia Institute of Technology The George W. Woodruff School of Mechanical Engineering Nuclear & Radiological Engineering/Medical Physics Program Ph.D. Qualifier Exam Fall Semester 007 Your ID Code Radiation

More information