Georgia Institute of Technology. Radiation Physics (Day 1)

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

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

neutrons in the few kev to several MeV Neutrons are generated over a wide range of energies by a variety of different processes.

Radiation Quantities and Units

Class XII Chapter 13 - Nuclei Physics

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


Physics of Radiotherapy. Lecture II: Interaction of Ionizing Radiation With Matter

Chapter Four (Interaction of Radiation with Matter)

Nuclear Physics and Astrophysics

Physics 3204 UNIT 3 Test Matter Energy Interface

LECTURE 26 RADIATION AND RADIOACTIVITY. Instructor: Kazumi Tolich

State the main interaction when an alpha particle is scattered by a gold nucleus

MCRT L8: Neutron Transport

Interaction of Ionizing Radiation with Matter

Chapter V: Interactions of neutrons with matter

CHARGED PARTICLE INTERACTIONS

Physics 202H - Introductory Quantum Physics I Midterm Test - A - Solutions

Nuclear Spectroscopy: Radioactivity and Half Life

Exam, FK5024, Nuclear & particle physics, astrophysics & cosmology, October 26, 2017

Thursday, April 23, 15. Nuclear Physics

Interaction of Particles and Matter

PhysicsAndMathsTutor.com 1

Atomic and nuclear physics

Nuclear Binding, Radioactivity

General Physics (PHY 2140)

Interactions of Particulate Radiation with Matter. Purpose. Importance of particulate interactions

Unit 6 Modern Physics

Physic 492 Lecture 16

Nuclear Physics. PHY232 Remco Zegers Room W109 cyclotron building.

There are 82 protons in a lead nucleus. Why doesn t the lead nucleus burst apart?

The interaction of radiation with matter

Introduction to Radiological Sciences Neutron Detectors. Theory of operation. Types of detectors Source calibration Survey for Dose

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

Part II Particle and Nuclear Physics Examples Sheet 4

(10%) (c) What other peaks can appear in the pulse-height spectrum if the detector were not small? Give a sketch and explain briefly.

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

Particle Interactions in Detectors

SOURCES of RADIOACTIVITY

Possible Interactions. Possible Interactions. X-ray Interaction (Part I) Possible Interactions. Possible Interactions. section

[2] State in what form the energy is released in such a reaction.... [1]

Interactions with Matter Photons, Electrons and Neutrons

Write down the nuclear equation that represents the decay of neptunium 239 into plutonium 239.

Alpha Decay. Decay alpha particles are monoenergetic. Nuclides with A>150 are unstable against alpha decay. E α = Q (1-4/A)

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

Radioactivity III: Measurement of Half Life.

The number of protons in the nucleus is known as the atomic number Z, and determines the chemical properties of the element.


Units and Definition

UNIVERSITY OF CAPE TOWN. EEE4101F / EEE4103F: Basic Nuclear Physics Problem Set 04. Due 12:00 (!) Wednesday 8 April 2015

Physics 102: Lecture 28

Cross-Sections for Neutron Reactions

1. This question is about the Rutherford model of the atom.

Nuclear Chemistry. Decay Reactions The most common form of nuclear decay reactions are the following:

NUCLEAR PHYSICS. Challenging MCQ questions by The Physics Cafe. Compiled and selected by The Physics Cafe

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

9 Nuclear decay Answers to exam practice questions

Neutron interactions and dosimetry. Eirik Malinen Einar Waldeland

Introduction to Nuclear Engineering

UNIT 13: NUCLEAR CHEMISTRY

6 Neutrons and Neutron Interactions

Introduction to Nuclear Science

[1] (c) Some fruits, such as bananas, are naturally radioactive because they contain the unstable isotope of potassium-40 ( K.

ASSESSMENT UNIT PH5: FIELDS, FORCES AND NUCLEI. A.M. WEDNESDAY, 11 June hours

(a) (i) State the proton number and the nucleon number of X.

CHAPTER 12 TEST REVIEW

Week 2: Chap. 2 Interaction of Radiation

Page 1. ConcepTest Clicker Questions Chapter 32. Physics, 4 th Edition James S. Walker

Chapter 29. Nuclear Physics

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

Lecture 33 Chapter 22, Sections 1-2 Nuclear Stability and Decay. Energy Barriers Types of Decay Nuclear Decay Kinetics

III. Energy Deposition in the Detector and Spectrum Formation

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

Physics Assessment Unit A2 1

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

The Compton Effect. Martha Buckley MIT Department of Physics, Cambridge, MA (Dated: November 26, 2002)

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

LECTURE 23 NUCLEI. Instructor: Kazumi Tolich

Nuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic

Nice Try. Introduction: Development of Nuclear Physics 20/08/2010. Nuclear Binding, Radioactivity. SPH4UI Physics

Atomic and Nuclear Radii

NUCLEI, RADIOACTIVITY AND NUCLEAR REACTIONS

1 v. L18.pdf Spring 2010, P627, YK February 22, 2012

Interaction theory Photons. Eirik Malinen

NJCTL.org 2015 AP Physics 2 Nuclear Physics

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?

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

Physics 102: Lecture 26. X-rays. Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1

Compound and heavy-ion reactions

Chapter from the Internet course SK180N Modern Physics

Ch05. Radiation. Energy and matter that comes from the nucleus of an atom. version 1.6

Chapter 44 Solutions. So protons and neutrons are nearly equally numerous in your body, each contributing mass (say) 35 kg:

Radioactivity. General Physics II PHYS 111. King Saud University College of Applied Studies and Community Service Department of Natural Sciences

Examination Radiation Physics - 8N120, 2 November

u d Fig. 6.1 (i) Identify the anti-proton from the table of particles shown in Fig [1]

Chemical Engineering 412

CHARGED PARTICLE IONIZATION AND RANGE

PHYS 5012 Radiation Physics and Dosimetry

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]

The Atomic Nucleus. Bloomfield Sections 14.1, 14.2, and 14.3 (download) 4/13/04 ISP A 1

Transcription:

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 Physics (Day 1) Instructions 1. Use a separate page for each answer sheet (no front to back answers).. The question number should be shown on each answer sheet. 3. ANSWER OF 6 QUESTIONS ONLY.. Staple your question sheet to your answer sheets and turn in.

NRE/MP Radiation Physics Answer any of the following 6 questions: 1. A gold foil weighing 3.5 mg is irradiated by a thermal-neutron flux density of 10 13 n cm - s -1. The interaction cross section is σ = 96 10 - cm /atom, and the half-life, τ 1/ =.70 d for 198 Au. The value of Avogadro s constant is 6.03 10 3 atoms/mole. The gram-atomic weight of gold is 197.0 g/mole. One curie (1 Ci) is 3.7 10 10 Bq. a) How long will it take for the foil to achieve an activity of 100 mci of 198 Au? b) What is the equilibrium level of activity? c) How long would it have taken to reach the same activity if the decay of 198 Au were negligible during that time? d) What is the true activity reached at that time?. Answer the following questions regarding photon interactions with media. State your assumptions if necessary. a) Is the Compton mass attenuation coefficient larger in carbon (Z= 6; A=1) or lead (Z=8; A=07)? Why? b) On the basis of the Klein-Nishna theory, what is the ratio of the Compton interaction cross sections per atom for lead and carbon? c) Suppose two photons with hν = and 0 MeV, respectively, undergo pair production interactions with a medium. What is the average energy of the charged particles resulting from pair production in the nuclear field for each photon? What is the average energy of the charged particles resulting from pair production in the electron field (i.e., triplet production) for each photon? 3. Answer the following questions regarding charged particle interactions with media. State your assumptions if necessary. a) Compare the passage of charged and uncharged particles through matter. What is the approximate probability of a single charged particle achieving a pathlength equal to twice its range? What is the approximate probability of a single photon having a pathlength twice as great as the mean free path 1/μ (Assume the photon is totally absorbed in its first interaction). b) Briefly describe the general types of interactions that contribute to the collision stopping power, (dt/ρdx) c.. The semi-empirical nuclear binding energy formula is given below: where / 3 1/ 3 1 A a A a3z A a ( N Z) B = a A ± a A a 1 5 1/ = 15.56 MeV, a = 17.3 MeV, a3 = 0.7 MeV, a = 3.8 MeV, and a5 1. 0 MeV 1 = (a) Explain the physical meaning of each of the five terms in the above formula.

(b) Use the formula to calculate the mass of m n = p 08 8 Pb 1.008665 u, m = 1.007765 u, and 1u = 931. 9 MeV nucleus. Other data needed: (c) Discuss the discrepancy between your result of (b) and that shown in Attachment A. 5. In an alloyed Pu(Be) neutron source, neutrons are produced from the interactions of alpha particles (emitted from 38 Pu) with the 9 Be nuclei. That is, and 38 9 Pu 3 U + 1 Be+ He 0 n+ He 1 6 C (a) Use the mass table (Attachment A) to calculate the kinetic energy of the alpha particle. 1/ 3 e (b) Given that the nuclear radius obeys the formula, R = 1.5 A fm and that = 1. πε 0 MeV fm, use the classical approach to estimate the coulomb barrier (in MeV) for the above (α,n) reaction. (c) Use the classical approach to estimate the cross section (in barns) for the above (α,n) reaction, and discuss how the cross section should be modified by the quantummechanical approach. 6. The first resonance is observed at E n =.077 MeV in the neutron total cross section for 1 1 13 0 n+ C C in a laboratory experiment. (a) What energy, measured from the ground state of 13 C, is the excited state which gives rise to the above resonance? (b) If the total width (Γ) of the resonance is 8 kev, what is the most probable reaction type of this resonance? e.g. (n,γ), (n, elastic), (n, inelastic),.. etc. Why? 3

5