PhD Qualifying Exam Nuclear Engineering Program. Part 1 Core Courses

Similar documents
PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY

Radiation and Radioactivity. PHYS 0219 Radiation and Radioactivity

Chapter 18: Radioactivity And Nuclear Transformation. Presented by Mingxiong Huang, Ph.D.,

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

QUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter

Examination Radiation Physics - 8N120, 2 November

Chapter 21. Preview. Lesson Starter Objectives Mass Defect and Nuclear Stability Nucleons and Nuclear Stability Nuclear Reactions

Physics 3204 UNIT 3 Test Matter Energy Interface

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

Chemical Engineering 412

Chapter 21 Nuclear Chemistry

Neutron Dose near Spent Nuclear Fuel and HAW after the 2007 ICRP Recommendations

Nuclear Chemistry. The Nucleus. Isotopes. Slide 1 / 43. Slide 2 / 43. Slide 3 / 43

What do we know from GCSE?

Physics 30: Chapter 8 Exam Nuclear

Examination Radiation Physics - 8N120 5 November 2014, 13:30-16:30

Name Date Class NUCLEAR RADIATION. alpha particle beta particle gamma ray

Nuclear fission is used in nuclear power stations to generate electricity. Nuclear fusion happens naturally in stars.

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

Lab 14. RADIOACTIVITY

2. The Steady State and the Diffusion Equation

Natural Radiation K 40

LECTURE 26 RADIATION AND RADIOACTIVITY. Instructor: Kazumi Tolich

NUCLEI, RADIOACTIVITY AND NUCLEAR REACTIONS

Units and Definition

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

Alpha-energies of different sources with Multi Channel Analyzer (Item No.: P )

EXPERIMENT FOUR - RADIOACTIVITY This experiment has been largely adapted from an experiment from the United States Naval Academy, Annapolis MD

Chapter 30 Nuclear Physics and Radioactivity

RADIOACTIVITY Q32 P1 A radioactive carbon 14 decay to Nitrogen by beta emission as below 14 x 0

Class XII Chapter 13 - Nuclei Physics

Nuclear Spectroscopy: Radioactivity and Half Life

Quality Assurance. Purity control. Polycrystalline Ingots

Alpha-Energies of different sources with Multi Channel Analyzer

Radiation Detection. 15 th Annual OSC Readiness Training Program.

22.01 Fall 2015, Quiz 1 Solutions

Nuclear Physics and Astrophysics

Radioactivity III: Measurement of Half Life.

SECTION 8 Part I Typical Questions

The basic structure of an atom is a positively charged nucleus composed of both protons and neutrons surrounded by negatively charged electrons.


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

Workout Examples No.of nucleons Binding energy

UNIVERSITY OF SOUTHAMPTON

Chapter 21. Chemistry, The Central Science, 10th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten


Quiz, Physics & Chemistry

CHAPTER 12 TEST REVIEW

4.4.1 Atoms and isotopes The structure of an atom Mass number, atomic number and isotopes. Content

Examination cover sheet

Nuclear Physics Lab I: Geiger-Müller Counter and Nuclear Counting Statistics

Radioactivity & Nuclear. Chemistry. Mr. Matthew Totaro Legacy High School. Chemistry

B. Rouben McMaster University Course EP 4D03/6D03 Nuclear Reactor Analysis (Reactor Physics) 2015 Sept.-Dec.

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

SOURCES of RADIOACTIVITY

Name: Class: Date: SHORT ANSWER Answer the following questions in the space provided.

Radiation Detection and Measurement

2007 Fall Nuc Med Physics Lectures

RADIOACTIVITY MATERIALS: PURPOSE: LEARNING OBJECTIVES: DISCUSSION:

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

Lesson 6: Diffusion Theory (cf. Transport), Applications

Chapter 12: Nuclear Reaction

Minnesota Science Olympiad Division C University of Minnesota Regional Saturday, February 3, 2007

K 40 activity and Detector Efficiency

HOMEWORK 22-1 (pp )

DETECTORS. I. Charged Particle Detectors

Delayed neutrons in nuclear fission chain reaction

CH 222 Chapter Twenty-one Concept Guide

Aluminum Half-Life Experiment

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

EXPERIMENT 11: NUCLEAR RADIATION

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

Karlsruhe Nuclide Chart

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

Nuclear Physics. AP Physics B

17 Neutron Life Cycle

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

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

Interaction of the radiation with a molecule knocks an electron from the molecule. a. Molecule ¾ ¾ ¾ ion + e -

4.4 Atomic structure Notes

Introduction to Nuclear Engineering. Ahmad Al Khatibeh

Reactor Physics: Basic Definitions and Perspectives. Table of Contents

Chapter 18. Nuclear Chemistry

Radioactivity and Radioactive Decay

Radioactivity APPARATUS INTRODUCTION PROCEDURE

Identification of Naturally Occurring Radioactive Material in Sand

1.1 ALPHA DECAY 1.2 BETA MINUS DECAY 1.3 GAMMA EMISSION 1.4 ELECTRON CAPTURE/BETA PLUS DECAY 1.5 NEUTRON EMISSION 1.6 SPONTANEOUS FISSION

Nuclear Study Packet. 1. What subatomic particles are involved in nuclear reactions? 2. What subatomic particles are involved in chemical reactions?

Fundamentals of Radionuclide Metrology

EVALUATION OF PWR AND BWR CALCULATIONAL BENCHMARKS FROM NUREG/CR-6115 USING THE TRANSFX NUCLEAR ANALYSIS SOFTWARE

y loo Physics Essentials Workbook Stage 2 Physics Exercises

Part 12- Physics Paper 1 Atomic Structure Knowledge Questions

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

P7 Radioactivity. Student Book answers. P7.1 Atoms and radiation. Question Answer Marks Guidance

Cosmic Rays Detector. Use of Coincidence Detector for Measures of Cosmic Rays. Lodovico Lappetito. RivelatoreRaggiCosmici_ENG - 6/22/2015 Page 1

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]

Radioactivity One of the pieces of evidence for the fact that atoms are made of smaller particles came from the work of Marie Curie

Chapter Three (Nuclear Radiation)

ABC Math Student Copy

Compton Camera. Compton Camera

Transcription:

PhD Qualifying Exam Nuclear Engineering Program Part 1 Core Courses 9:00 am 12:00 noon, November 19, 2016

(1) Nuclear Reactor Analysis During the startup of a one-region, homogeneous slab reactor of size (a), placed in a vacuum, using the time-dependent, one-speed diffusion equation, 1 φ v t D 2 φ x 2 + Σ aφ(x, t) = ν Σ f φ(x, t) we obtain the flux formulation expressed by φ(x, t) = A n e λ nt cos (B n x) n odd Where λ n = vσ a + vdb 2 n v(ν Σ f ) and B n = nπ. Note that υ is neutron speed, and ν is average a number of neutrons per fission. a) If λ 1 >0, show that the flux approaches the first harmonic (i.e., n=1) after a short time. (18%) b) What is the material buckling for this reactor? (4%) c) What is the criticality condition for this reactor? (7%) d) Show that the probability of non-leakage is expressed by P NL = 1 (21%) 1+B 2 L 2 1 e) Show that the prompt neutron life-time is expressed by l p = (18%) vσ a (1+B 2 L 2 ) f) Show that λ 1 = (1 k) l p (25%) g) Using the expression in part (f), for a reactor with k = 1.003, using your guess for l p, how much the neutron flux change in 1 sec? Is this a stable reactor? (explain your answers) (7%)

(2) Reactor Thermal Hydraulics Consider a cylindrical nuclear fuel rod of length L and diameter d f that is encased in a concentric tube. Pressurized water flows through the annular region between the rod and the tube at a rate of m, and the outer surface of the tube is well insulated. Heat generation occurs within the fuel rod, and the volumetric heat generation rate along the rod is given by: where q o W/m 3 is a constant. sin / q x q x L, o A uniform convection coefficient h may be assumed to exist between the surface of the rod and the water flow. Axial conduction can be neglected in rod and fluid. The specific heat of water c p, and the thermal conductivity of the fuel rod k f are constants. The system is in steady state condition. r Coolant T, m, c i p 0 x Fuel rod, d, k q q sin x / L o f f L a) Obtain expressions for the local heat flux q " and the total heat transfer rate q from the fuel rod to the water. [15%] b) The mean temperature of the water at the inlet is T i. Obtain an expression for the variation of the mean temperature T (x) of the water with distance x along the tube. [20%] c) Obtain an expression for the variation of the rod surface temperature T s (x) with distance x along the tube. Develop an expression for the x location at which this temperature is maximized. [30%] d) Obtain an expression for the variation of the temperature inside the fuel rod T f (x, r) with distance x along the tube and radial distance r from the centerline. Develop an expression for the location (x, r) at which T f (x, r) is maximized. Assume the temperature distribution is axisymmetric in the fuel rod, and the axial heat conduction can be neglected. [35%] Hint: the Laplacian operator in the cylindrical coordinate system can be given as: 1 1 r r r r x 2 2 2 r 2 2 2

(3) Advanced Nuclear Materials Answer the following questions: a) Describe thermal spikes mechanism? (20%). b) What is the effect of neutron radiation on the material yield strength? Describe the mechanism. (20%) c) Where does He atom come from in fuel cladding? (20%) d) What is embrittlement? Where does this problem come from? (20%). e) Describe the threshold energy required to displace an atom under neutron irradiation? (20%).

(4) Radiation Detection and Shielding Half-life of a Long-lived Radionuclide: The following experiment was then conducted to measure the K-40 half-life. 300.0 ± 0.1 mg of reagentgrade potassium chloride (KCl) was measured out in a 2.5 cm diameter planchette. The planchette was placed 1 cm away from the window of a Geiger-Mueller detector. The Geiger-Mueller detector window has a diameter of 3 cm. The effective solid angle averaged over the surface of the sample presented to the detector is 2.336 steradians. The sample and G-M counter are located inside a container shielded by 4-cm of lead. A 30-minute background count rate is determined before and after counting the sample. The two background counts are averaged. For this experiment, the average background count rate was 3.5 ± 0.3 cpm. The KCl sample was then counted for four hours obtaining a total of 11,621 counts. The following data is provided: Abundance of 40 K in natural potassium, 40 : 1.17 x 10-4. The gram-atomic weight of 40 K is 39.9640 g/mole. The gram-molecular weight of KCl is 74.5513 g/mole. 40 K undergoes beta-minus decay 89.28% of the time with an average beta energy of 560.18 kev and max beta energy of 1311.07 kev. It also undergoes electron capture decay 10.67% of the time releasing a gamma-ray of energy 1460.82 kev. The Geiger-Mueller detector has an efficiency of counting beta particles at 98%. Its efficiency for counting gamma-rays at 1460 kev, however, is essentially zero. Loss due to absorption of soft beta-rays in the mica window of the Geiger-Mueller detector is estimated to be 5%. a) Using the provided information calculate the half-life of 40 K in years. (40%) b) Assuming the only uncertainties are the background count rate, the total sample count, and the measurement of the KCl mass, estimate the expected standard deviation of the half-life value in years. (60%)

(5) Advanced Engineering Mathematics The Maxwellian density function expressed by M(E, T) = 4π ( m 2πkT ) 3/2 v 2 e mv2 2kT Where, m is mass, k is the Boltzmann constant, T is temperature in Kelvin, and v is speed. a) Derive the density function in terms of kinetic energy (E) (33%) b) Show that the most probable energy does not correspond to the most probable speed (38%) c) Determine the average energy (29%)

PhD Qualifying Exam Nuclear Engineering Program Part 2 Specialty Courses Radiation Detection & Shielding 2:00 pm 5:00 pm, November 19, 2016

Specialty - Radiation Detection & Shielding (1) (37.5%) Transient Equilibrium When the half-life of the parent is slightly greater than that of the daughter, transient equilibrium can occur. In this situation, the daughter activity builds up to a maximum and then decays away. a) For the case where you have the decay chain X 1 X 2 X 3 where X 3 is stable, starting out with 100% of the parent X 1 with an initial activity A 1,0, derive an equation for the total radioactivity of the parent plus the daughter with time, i.e. A tot (t) = A 1 (t) + A 2 (t). (65%) b) Derive an expression for the time at which the total activity derived above reaches a maximum. (35%)

Specialty - Radiation Detection & Shielding (2) (37.5%) A 1-Ci point source of 24 Na is to be stored in a lead box. The radionuclide emits two photons per disintegration with energies of 2.75 MeV and 1.37 MeV in decaying by β emission to stable 24 Mg. How thick must the lead walls on the box be such that the exposure rate 1 meter away from the 1-Ci point source is less than 2 mr/hr? The exposure rate, X, can be calculated by: X = Γ α d 2, where α is the activity in millicuries of the point source, d is the distance in centimeters from the point source, and Γ is exposure rate constant from the Table below. Density of lead = 11.4 g/cm 3 See next page

Specialty - Radiation Detection & Shielding (3) (25%) Radiation Detector Operation Discuss the following topics/concepts related to a radiation detector: a) Draw the gas multiplication curve as a function of pulse height versus applied voltage. (15%) b) Using the different regions of the gas multiplication curve above explain the operation of applicable gas-filled detectors and how these detectors take advantage of the features of this curve to work. Include a detailed description of these detectors. (50%) c) Indicate how the gas multiplication curve in part (a) above would change for an incoming alpha particle versus the curve for an incoming beta particle. Explain why the curve changes the way it does. (10%) d) Explain how a semiconductor diode detector works to detect radiation. In your explanation, include the reason reverse bias is used. (25%)

PhD Qualifying Exam Nuclear Engineering Program Part 2 Specialty Courses Particle Transport Methods and Reactor Physics 2:00 pm 5:00 pm, November 19, 2016

Specialty - Particle Transport Methods and Reactor Physics (1) (25%) A one-region slab of size a is placed in a vacuum. An anisotropic planar source is placed on the left boundary of the slab as depicted below vacuum D Σ a vacuum Source The angular source is expressed by S(Ω ) = S 0 ( 1 4π + 1 8π μ) Where, Ω is unit vector particle direction, and μ is direction cosine of polar angle corresponding to direction Ω. Derive a formulation for neutron flux distribution in the slab using the one-speed diffusion equation. Hint: The one-speed diffusion equation is given by D d2 φ + Σ dx aφ(x) = S(x), 2 and partial current formulations based on the diffusion approximation are expressed by a J ± (x) = φ(x) 4 D 2 dφ(x) dx

Specialty Particle Transport Methods and Reactor Physics (2) (37.5%) The one speed, 1-D transport equation in the Cartesian geometry is given by μ ψ(x,μ) x 1 + σ t ψ(x, μ) = 2π dμ σ s (x, μ 0 )ψ(x, μ ) 1 + S(x, μ), a) Derive expressions of the scattering and source terms if both scattering and source are isotropic (23%) b) Derive the one-speed, 1-D discrete ordinates (S N ) equations (Do not need to perform spatial discretization) (13%) c) Discuss a methodology for determining the S N quadrature set in a 1-D geometry (37%) d) To derive the P L equations, briefly explain the procedure/formulation you would use (Do NOT derive the P L equations.) (13%) e) Under what conditions the P L and S N equations are equivalent? (7%) f) What is the difficulty with the P L equations? (7%)

Specialty- Particle Transport Methods and Reactor Physics (3) (37.5%) The Monte Carlo method is used for solving an integral such as b I = dxf(x)g(x) a a) Explain the standard procedure and formulation used to solve the above integral (17%) b) Briefly explain the importance sampling method for solving an integral (10%) c) Derive the theoretical variance corresponding to the following integral (17%) 1 dx(1 x 2 ) 0 d) Using the importance sampling approach, propose an effective pdf (f (x)) to solve the integral in part c, and derive the corresponding variance (40%) e) Compare the results of the parts c and d (3%) f) Name two other variance reduction techniques for solving the above integral; which component of the integral is modified in these techniques? (Do not solve the integral with these techniques) (13%)