Examination Radiation Physics - 8N120, 2 November

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

Examination cover sheet

If you cannot solve the whole problem, write down all relevant equations and explain how you will approach the solution. Show steps clearly.

Class XII Chapter 13 - Nuclei Physics


Slide 1 / 57. Nuclear Physics & Nuclear Reactions Practice Problems

There are a number of experimental observations that could not be explained by classical physics. For our purposes, the main one include:

Physics 3204 UNIT 3 Test Matter Energy Interface

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

Physics 208 Exam 3 Nov. 28, 2006

Physics 280 Quantum Mechanics Lecture

The wavefunction ψ for an electron confined to move within a box of linear size L = m, is a standing wave as shown.

SCHOOL OF HEALTH AND APPLIED SCIENCES DEPARTMENT OF NATURAL AND APPLIED SCIENCES BSC PROGRAMME

Multiple Choice Questions

Physics 107 Final Exam May 6, Your Name: 1. Questions

Basic science. Atomic structure. Electrons. The Rutherford-Bohr model of an atom. Electron shells. Types of Electrons. Describing an Atom

Sharif University of Technology Physics Department. Modern Physics Spring 2016 Prof. Akhavan

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

PHYSICS 250 May 4, Final Exam - Solutions

normalized spectral amplitude R(λ)

Atomic and Nuclear Radii

Physics 342: Modern Physics

Quantum Physics (PHY-4215)

MIDTERM 3 REVIEW SESSION. Dr. Flera Rizatdinova

Department of Natural Sciences Clayton State University. Physics 3650 Quiz 1

PHYSICS Thermodynamics and Modern Physics. Practice Final Exam. Fall 2011

Physics 3223 Solution to Assignment #5

11 Quantum theory: introduction and principles

MIDSUMMER EXAMINATIONS 2001 PHYSICS, PHYSICS WITH ASTROPHYSICS PHYSICS WITH SPACE SCIENCE & TECHNOLOGY PHYSICS WITH MEDICAL PHYSICS

IB Physics SL Y2 Option B (Quantum and Nuclear Physics) Exam Study Guide Practice Problem Solutions

UNIVERSITY OF SWAZILAND

REDEFINING IONISATION ENERGY OF AN H-ATOM PART 1. Elementary charge associated with a photon x C

CHEM121H Honors General Chemistry 1 October 5, Hour Exam #1

Physics 126 Practice Exam #4 Professor Siegel


1 (a) Sketch the electric field surrounding the gold nucleus drawn below. (3)

Instead, the probability to find an electron is given by a 3D standing wave.

Final Exam Practice Solutions

Atoms, nuclei, particles

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

Chapter 27 Early Quantum Theory and Models of the Atom Discovery and Properties of the electron

Lecture 32 April

Introduction to Nuclear Physics and Nuclear Decay

Atomic and nuclear physics

CHAPTER 12 TEST REVIEW

Chapter 39. Particles Behaving as Waves

Thursday, April 23, 15. Nuclear Physics

Rb, which had been compressed to a density of 1013

Properties of Light and Atomic Structure. Chapter 7. So Where are the Electrons? Electronic Structure of Atoms. The Wave Nature of Light!

2013 CAP Prize Examination

is the minimum stopping potential for which the current between the plates reduces to zero.

Lecture 1. Introduction to Nuclear Science

THE UNIVERSITY OF PRETORIA

Z is the atomic number, the number of protons: this defines the element. Isotope: Nuclides of an element (i.e. same Z) with different N.

PHYS 3313 Section 001 Lecture #14

Slowing down the neutrons

CHAPTER 5. The Structure of Atoms

Fall 2012 Qualifying Exam. Part I

Quantum Mechanics. Reilly V. Bautista. September 5, Reilly V. Bautista Quantum Mechanics September 5, / 78

Final Exam - Solutions PHYS/ECE Fall 2011

1 Stellar Energy Generation Physics background

Introduction to Nuclear Reactor Physics

Graduate Written Examination Fall 2014 Part I

Physics 1C. Lecture 29A. "Nuclear powered vacuum cleaners will probably be a reality within 10 years. " --Alex Lewyt, 1955

Exam 2 Development of Quantum Mechanics

Chapters 31 Atomic Physics

Chapter 1 The Bohr Atom

LECTURE 23 SPECTROSCOPY AND ATOMIC MODELS. Instructor: Kazumi Tolich

MEMORIAL UNIVERSITY OF NEWFOUNDLAND DEPARTMENT OF PHYSICS AND PHYSICAL OCEANOGRAPHY. PHYSICS 2750 FINAL EXAM - FALL December 13, 2007

Absorber Alpha emission Alpha particle Atom. Atomic line spectra Atomic mass unit Atomic number Atomic structure. Background radiation

Planck s Quantum Hypothesis Blackbody Radiation

PHY 571: Quantum Physics

2007 Fall Nuc Med Physics Lectures

UNM Physics 262, Fall 2006 SAMPLE Midterm Exam 3: Quantum Mechanics

Lecture 4. The Bohr model of the atom. De Broglie theory. The Davisson-Germer experiment

Physics 102: Lecture 24. Bohr vs. Correct Model of Atom. Physics 102: Lecture 24, Slide 1

GRADUATE WRITTEN EXAMINATION. Fall 2018 PART I

Chapter 44. Nuclear Structure

SECTION A Quantum Physics and Atom Models

A fluorescent tube is filled with mercury vapour at low pressure. After mercury atoms have been excited they emit photons.

January 2017 Qualifying Exam

PHY293 Lecture #9. df hf

Lesson 1. Introduction to Nuclear Science

Atomic Structure and Processes

University of California, Berkeley Physics H7C Spring 2011 (Yury Kolomensky) THE FINAL EXAM Monday, May 9, 7 10pm. Maximum score: 200 points

Unit 6 Modern Physics

Electronic Structure of Atoms. Chapter 6

Chapter 1. From Classical to Quantum Mechanics

CHAPTER 7 TEST REVIEW

NJCTL.org 2015 AP Physics 2 Nuclear Physics

Chemistry 201: General Chemistry II - Lecture

August 2013 Qualifying Exam

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

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

Physics GRE: Atomic Physics. G. J. Loges 1. University of Rochester Dept. of Physics & Astronomy. xkcd.com/658/

Z is the atomic number, the number of protons: this defines the element. Isotope: Nuclides of an element (i.e. same Z) with different N.

August 2013 Qualifying Exam. Part II

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

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

Physics 100 PIXE F06

Transcription:

Examination Radiation Physics - 8N0, November 0-4.00-7.00 Four general remarks: This exam consists of 6 assignments on a total of pages. There is a table on page listing the maximum number of that can be achieved in each assignment. You are not allowed to use books, notes, lecture notes, notebooks, telephones, tablets etc during the exam. It is allowed to use a ordinary calculator. You can use the appended list of constants and formulas during the exam. All answers should be formulated and motivated clearly.. (a) What is the energy in electron-volt of a photon with a wavelengths of 550 nm? (b) How many photons are emitted each second by a 5 watt LED lamp, that emits only photons of 550 nm? You may assume that all the energy used by the lamp is transferred to the photons.. Consider the Compton effect where an incoming photon with an energy of.0 MeV interacts with a free electron. The trajectory of the scattered photon has an angle θ = 80 with respect to the trajectory of the incoming photon. (a) Compute the wavelength of the incoming photon. (b) Compute the wavelength and energy of the scattered photon. Next we consider the Compton effect for an incoming photon with an energy of 0.0 MeV, that is again scattered by an angle θ = 80 with respect to the trajectory of the incoming photon. (c) Compute the wavelength of the incoming photon. (d) Compute the wavelength and energy of the scattered photon. The effect where an incoming photon is scattered over an angle of (approximately) 80 is called Compton backscattering. (e) What is in the case of Compton backscattering the maximal energy of the scattered photon? Hint: Look at incoming photons with very high energy.. Suppose an electron is trapped in a region ( the hydrogen atom ) of width x = a 0, where a 0 = 0.059 nm is the Bohr radius. (a) What is the uncertainty of the velocity in the x direction of this electron? (b) What is in the Bohr model the velocity of an electron in the ground state of hydrogen? Hint: For a circular orbit mv = E, where E is the energy of the electron.

4. In this exercise we consider a one-dimensional particle with mass m that can only move along the positive x-axis (so 0 < x < ), in a potential U(x) = q x, where q is a positive constant. This potential occurs for instance if the particle has an electric charge and is attracted by another electric charge that is fixed in x = 0. (a) Give the Schrödinger equation for this case. Given is that a solution of the Schrödinger equation for this case is of the form Ψ(x) = A x e ax. (b) Compute the first and second derivative of this wave function. (c) Substitute Ψ(x) and the second derivative of Ψ(x) in the Schrödinger equation. By considering the coefficients of e ax and x e ax we obtain two equations, from which a and E can be found. Give these two equations. (d) Solve these two equations and give the corresponding energy value E and the corresponding wave function Ψ(x). (e) The constant A is not yet known. Which condition for the wave function Ψ(x) can be used to find A? (f) Compute the value of A. You may use that 0 x n e bx dx = n!/b n+, for integer n 0 and b > 0. 5. Consider the α emission A ZX A 4 Z Y + α. (a) Give the Q-value of this expression, expressed in nuclear masses. Use A ˆM Z for the nuclear mass and A ZM for the corresponding atomic mass. (b) Show how this Q-value can be rewritten in terms of atomic masses. (c) Assuming that the mother X has no kinetic energy before the reaction and that all of the decay energy is distributed between the α-particle and daughter nucleus Y, derive the formulas that gives the distribution of Q between α-particle and daughter. Give the actual kinetic energies of the α-particle and of the daughter nucleus. 6. Consider the part of the nuclides chart in Figure. (a) Give the three possible beta decay reaction from 98 Au and compute the Q-values for these three forms of beta decay. (b) Which of these three beta decays are energetically possible? (c) Following the information on the chart of nuclides, only one of these beta decay reactions is observed experimentally. Which reaction is that? (d) Explain which combinations of successive decay processes on the nuclides chart corresponds approximately with this beta decay reaction. (Note : use the right part of the 98 Au entry in the chart; the left part describes excited states of 98 Au. Note : on the nuclides chart the energies of alpha and beta decay are indicted in MeV, the energies of gamma decays are in kev.)

Figuur : part of the nuclides chart for assignment 6 Points: (total 60) a: b: 5a: 5b: 5c: 4a: 4b: 4c: 4d: 4e: 4f: point point a: b: c: d: e: 6 a: b: 4 4 6a: 6b: 6c: 6d: point

4

Radiation Physics - 8N0 Formulas and constants - 0/0 physical constants: h = 6.66 0 4 Js (Planck s constant) k B =.8 0 J/K (Boltzmann s constant) c =.998 0 8 m/s (speed of light) e =.60 0 9 C (elementary charge) σ = 5.67099 0 8 W/(m K 4 ) (Stefan-Boltzmann constant) N a = 6.0 0 mole (Avogadro s constant) V m =.4 liter (at atm, 0 C) (Molair volume R =.097 0 7 m (Rydberg constant) µ B = 9.74 0 4 J/T (Bohr magneton) ɛ 0 = 8.854 0 F/m (vacuum permittivity) a 0 = 0.059 0 9 m = 0.059 nm (Bohr radius) hydrogen ionization energy=.6 ev unit conversions: ev =.60 0 9 J (electron-volt to Joule) J = 6.4 0 8 ev (Joule to electron-volt) u=.66056 0 7 kg = 9.5 MeV/c (atomair mass unit to kg to energy) hc = 40 ev nm (hc in electronvolt nanometer) masses: m e = 9.09 0 kg =0.000549 u =5 kev/c (mass of electron) m p =.67 0 7 kg =.007766 u m n =.675 0 7 kg =.0086654 u (mass of proton) (mass of neutron) M( H) = M =.00785 u (mass of hydrogen atom) M( 4 He) = 4 M = 4.00605 u (mass of helium atom) M( 98 80 M( 98 79 M( 98 78 Hg) = 98 80 M = 97.966769 u (mass of mercury isotope) Au) = 98 79 M = 97.9684 u (mass of gold isotope) Pt) = 98 78 Photons and radiation laws: M = 97.96789 u (mass of platinium isotope) λ ν = c E = hν λ max T =.898 0 mk R(λ) = 8π λ 4 kt c 4 R(λ) = c 8π hc 4 λ 4 λ I = σt 4 e hc/(λk BT ) (relation wave length frequency) (energy of photon) (Wien s displacement law) (radiation law of Rayleigh Jeans) (Planck s radiation law) (law of Stefan Boltzmann)

Fotoelectric effect and Compton effect: hf = ev s + φ λ λ = h ( cos(θ)) m e c (foto electric equation) (Compton scattering) Relativistic energy and impuls: E = (mc ) + (p c) p = mv v /c Atom model of Bohr: f = cr ( n m ) (Rydberg formula) r n = a 0 n = 4π h m e e E n = (4πɛ 0 ) me 4 h n =.6 n ev (radius nth orbit) (energy of nth orbit of hydrogen E n =.6Z n ev (idem, for other atoms (ions) with one electron) Wave mechanics: λ = h p h d Ψ + UΨ = EΨ m dx x p x h E t h (De Broglie wave length) (-dim. Schrödinger equation) (uncertainty relationship) (uncertainty relationship) Nuclear physics: R = r 0 A / (radius on nucleus) B tot (A, Z) = ZM H + (A Z)M n A ZM (binding energy) Q = (m initial m final ) c (Q-value) Some codings on the Chart of Nuclids: β + : beta plus decay, ɛ : electron capture, β : beta minus decay, α : alpha decay