Ba (Z = 56) W (Z = 74) preferred target Mo (Z = 42) Pb (Z = 82) Pd (Z = 64)

Size: px
Start display at page:

Download "Ba (Z = 56) W (Z = 74) preferred target Mo (Z = 42) Pb (Z = 82) Pd (Z = 64)"

Transcription

1 Produced by accelerating electrons with high voltage and allowing them to collide with metal target (anode), e.g, Tungsten. Three Events (Two types of x-ray) a) Heat X-Ray Tube b) bremsstrahlung (braking radiation) c) characteristic radiation emission, Photoabsorption or photoelectric absorption is the dominant interaction mechanism in the soft X-ray regime and for the lower hard X-ray energies. At higher energies, Compton scattering dominates. Which of the materials should be used to produce soft X-ray and hard x rays? Ba (Z = 56) W (Z = 74) preferred target Mo (Z = 42) Pb (Z = 82) Pd (Z = 64) 12/20/16 1

2 What is the minimum energy of the e -beam in the X-ray tube If an electron is ejected from the K shell. The vacancy is filled with a second electron from the M shell. The produced photon is referred to as: The direct interaction of an incident electron with the nucleus of an atom results in X-ray production g -ray production

3 The Interaction of X-Rays with Matter Attenuation A process by which radiation loses power (reduce intensity) as it travels through matter due to the interaction with it. half-value-layer (HVL) is the thickness at which the intensity/energy is reduced by half Deferential Absorption The deference of absorption of radiation (x-ray) by deferent body tissues. e.g., image of the bone is produced because more x-rays are absorbed by bone than by the surrounding soft tissue. Resulted from - Transmitted x-ray through tissue. - Compton scattering by tissue. - Photoelectric effect. Depends on 1) Incident radiation (x-rays) energy. 2) Tissue atomic number. 3) Tissue mass density

4 The Interaction of X-Rays (high energy photon) with Matter Attenuation 1) As x-ray energy increases - Less Compton scattering - Slight increase in photoelectric interaction - More transmission through tissue Absorption edge: when the photon energy reaches the binding energy level for, e.g. E K, interaction with the K-shell electron becomes possible and the probability of photoelectric absorption jumps to a higher value; The K-absorption edge occurs at different photon energies with different materials.

5 The Interaction of X-Rays with Matter 2) As tissue atomic number increases - Very slight effect on Compton interaction - More photoelectric effect - Less x-ray transmission They depend on number of electrons, rather than, the mass number of the matter, the valency of a target matter, the free binding energy E K (kev), and the Molecular configuration. 3) As tissue mass density increases - Increase in Compton interaction - Increase in photoelectric interaction - Reduction in transmission through tissue Attenuation

6 Exponential decay

7

8 Ionizing and Non-Ionizing Radiation photons Non-ionizing Radiation Has enough energy to move atoms in the molecular range or cause vibrational or rotational excitations, but not enough to remove electrons. Uses - Microwave radiation for telecommunications and heating food - Infrared to provide heat - Radio waves for broadcasting

9 Secondary Electrons and Ionization Photons with enough energy can ionize atoms through the photoelectric and Compton effects Secondary electron: the recoiled electrons and photoelectrons set moving in the material; - Secondary electrons will have enough energy to ionize more atoms. - As they travel through the material they interact with the outer shells of the atoms and excite (ionize) them; Effects of Ionization - Air and gases become electrically conducting (the measurement of X- and gamma-rays); - Cause biological damage; - The excitation of atoms makes them emit light (luminescence); - Photographic effect (silver, bromide); - Heating of the material

10

11 Non-ionizing radiation may cause electrical shocks and burns Ionizing radiation produce general health effects, with variation with different tissue types. - damage the process of normal cell leading to cancer Natural sources of radiation in the environment - Background radiation: naturally occurs in our environment from earth, sun, our galaxy, other galaxies, and universe background. It is very low intensity. One CT scan can be equal to several years of background radiation exposure -Radon: colorless, odorless gas that comes from decaying rocks and soil; Accounts for half of annual exposure to radiation of average individual. Second leading cause of lung cancer after smoking. - Cosmic and terrestrial radiation: 8% of our average yearly exposure to radation, e.g., UV rays. UV rays can damage DNA in the skin and cause cancer.

Shell Atomic Model and Energy Levels

Shell Atomic Model and Energy Levels Shell Atomic Model and Energy Levels (higher energy, deeper excitation) - Radio waves: Not absorbed and pass through tissue un-attenuated - Microwaves : Energies of Photos enough to cause molecular rotation

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

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

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

LECTURE 4 PRINCIPLE OF IMAGE FORMATION KAMARUL AMIN BIN ABDULLAH

LECTURE 4 PRINCIPLE OF IMAGE FORMATION KAMARUL AMIN BIN ABDULLAH LECTURE 4 PRINCIPLE OF IMAGE FORMATION KAMARUL AMIN BIN ABDULLAH Lesson Objectives At the end of the lesson, student should able to: Define attenuation Explain interactions between x-rays and matter in

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

CHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH

CHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION CHAPTER 2 RADIATION INTERACTIONS WITH MATTER PREPARED BY: MR KAMARUL AMIN BIN ABDULLAH SCHOOL OF MEDICAL IMAGING FACULTY OF HEALTH SCIENCE Interactions

More information

Basic principles of x-ray production

Basic principles of x-ray production Production of X-Rays part 1 George Starkschall, Ph.D. Lecture Objectives Identify what is needed to produce x-rays Describe how a diagnostic x-ray tube produces x-rays Describe the types of interactions

More information

Physics of Radiography

Physics of Radiography Physics of Radiography Yao Wang Polytechnic Institute of NYU Brooklyn, NY 11201 Based on J L Prince and J M Links Medical Imaging Signals and Based on J. L. Prince and J. M. Links, Medical Imaging Signals

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 Radiotherapy. Lecture II: Interaction of Ionizing Radiation With Matter

Physics of Radiotherapy. Lecture II: Interaction of Ionizing Radiation With Matter Physics of Radiotherapy Lecture II: Interaction of Ionizing Radiation With Matter Charge Particle Interaction Energetic charged particles interact with matter by electrical forces and lose kinetic energy

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

FXA UNIT G485 Module X-Rays. Candidates should be able to : I = I 0 e -μx

FXA UNIT G485 Module X-Rays. Candidates should be able to : I = I 0 e -μx 1 Candidates should be able to : HISTORY Describe the nature of X-rays. Describe in simple terms how X-rays are produced. X-rays were discovered by Wilhelm Röntgen in 1865, when he found that a fluorescent

More information

Interaction of charged particles and photons with matter

Interaction of charged particles and photons with matter Interaction of charged particles and photons with matter Robert Miyaoka, Ph.D. Old Fisheries Center, Room 200 rmiyaoka@u.washington.edu Passage of radiation through matter depends on Type of radiation

More information

X-ray Interaction with Matter

X-ray Interaction with Matter X-ray Interaction with Matter 10-526-197 Rhodes Module 2 Interaction with Matter kv & mas Peak kilovoltage (kvp) controls Quality, or penetrating power, Limited effects on quantity or number of photons

More information

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

Possible Interactions. Possible Interactions. X-ray Interaction (Part I) Possible Interactions. Possible Interactions. section Possible Interactions X-ray Interaction (Part I) Three types of interaction 1. Scattering Interaction with an atom Deflected May or may not loss of energy 1 Possible Interactions Three types of interaction

More information

Basic physics of nuclear medicine

Basic physics of nuclear medicine Basic physics of nuclear medicine Nuclear structure Atomic number (Z): the number of protons in a nucleus; defines the position of an element in the periodic table. Mass number (A) is the number of nucleons

More information

CHAPTER 4 RADIATION ATTENUATION

CHAPTER 4 RADIATION ATTENUATION HDR202 PHYSICS FOR RADIOGRAPHERS 2 CHAPTER 4 RADIATION ATTENUATION PREPARED BY: MR KAMARUL AMIN BIN ABDULLAH SCHOOL OF MEDICAL IMAGING FACULTY OF HEALTH SCIENCES Learning Objectives At the end of the lesson,

More information

We have seen how the Brems and Characteristic interactions work when electrons are accelerated by kilovolts and the electrons impact on the target

We have seen how the Brems and Characteristic interactions work when electrons are accelerated by kilovolts and the electrons impact on the target We have seen how the Brems and Characteristic interactions work when electrons are accelerated by kilovolts and the electrons impact on the target focal spot. This discussion will center over how x-ray

More information

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney An Introduction to Diffraction and Scattering Brendan J. Kennedy School of Chemistry The University of Sydney 1) Strong forces 2) Weak forces Types of Forces 3) Electromagnetic forces 4) Gravity Types

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

Lecture 1 Bioradiation

Lecture 1 Bioradiation 1 1 Radiation definition: Radiation, when broadly defined, includes the entire spectrum of electromagnetic waves : radiowaves, microwaves, infrared, visible light, ultraviolet, and x-rays and particles.

More information

Sound wave bends as it hits an interface at an oblique angle. 4. Reflection. Sound wave bounces back to probe

Sound wave bends as it hits an interface at an oblique angle. 4. Reflection. Sound wave bounces back to probe : Ultrasound imaging and x-rays 1. How does ultrasound imaging work?. What is ionizing electromagnetic radiation? Definition of ionizing radiation 3. How are x-rays produced? Bremsstrahlung Auger electron

More information

ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM

ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM When white light passes through a prism, it spreads out into a rainbow of colours, with red at one end and

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

This watermark does not appear in the registered version - Laser- Tissue Interaction

This watermark does not appear in the registered version -  Laser- Tissue Interaction S S d Laser- Tissue Interaction Types of radiation ionizing radiation Non - ionizing radiation You may click on any of the types of radiation for more detail about its particular type of interaction

More information

Emphasis on what happens to emitted particle (if no nuclear reaction and MEDIUM (i.e., atomic effects)

Emphasis on what happens to emitted particle (if no nuclear reaction and MEDIUM (i.e., atomic effects) LECTURE 5: INTERACTION OF RADIATION WITH MATTER All radiation is detected through its interaction with matter! INTRODUCTION: What happens when radiation passes through matter? Emphasis on what happens

More information

X-RAY PRODUCTION. Prepared by:- EN KAMARUL AMIN BIN ABDULLAH

X-RAY PRODUCTION. Prepared by:- EN KAMARUL AMIN BIN ABDULLAH X-RAY PRODUCTION Prepared by:- EN KAMARUL AMIN BIN ABDULLAH OBJECTIVES Discuss the process of x-ray being produced (conditions) Explain the principles of energy conversion in x-ray production (how energy

More information

A Brief Introduction to Medical Imaging. Outline

A Brief Introduction to Medical Imaging. Outline A Brief Introduction to Medical Imaging Outline General Goals Linear Imaging Systems An Example, The Pin Hole Camera Radiations and Their Interactions with Matter Coherent vs. Incoherent Imaging Length

More information

1. Which of the following statements is true about Bremsstrahlung and Characteristic Radiation?

1. Which of the following statements is true about Bremsstrahlung and Characteristic Radiation? BioE 1330 - Review Chapters 4, 5, and 6 (X-ray and CT) 9/27/2018 Instructions: On the Answer Sheet, enter your 2-digit ID number (with a leading 0 if needed) in the boxes of the ID section. Fill in the

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

Electromagnetic radiation simply a stream of photons (a bundle of energy) What are photons???

Electromagnetic radiation simply a stream of photons (a bundle of energy) What are photons??? Electromagnetic radiation simply a stream of photons (a bundle of energy) What are photons??? no mass travel in a wave like pattern move at the speed of light contain a certain amount (or bundle) of energy

More information

Classical and Planck picture. Planck s constant. Question. Quantum explanation for the Wein Effect.

Classical and Planck picture. Planck s constant. Question. Quantum explanation for the Wein Effect. 6.1 Quantum Physics. Particle Nature of Light Particle nature of Light Blackbody Radiation Photoelectric Effect Properties of photons Ionizing radiation Radiation damage x-rays Compton effect X-ray diffraction

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

Atomic Physics. Chapter 6 X ray. Jinniu Hu 24/12/ /20/13

Atomic Physics. Chapter 6 X ray. Jinniu Hu 24/12/ /20/13 Atomic Physics Chapter 6 X ray 11/20/13 24/12/2018 Jinniu Hu 1!1 6.1 The discovery of X ray X-rays were discovered in 1895 by the German physicist Wilhelm Roentgen. He found that a beam of high-speed electrons

More information

Frequency: the number of complete waves that pass a point in a given time. It has the symbol f. 1) SI Units: Hertz (Hz) Wavelength: The length from

Frequency: the number of complete waves that pass a point in a given time. It has the symbol f. 1) SI Units: Hertz (Hz) Wavelength: The length from Frequency: the number of complete waves that pass a point in a given time. It has the symbol f. 1) SI Units: Hertz (Hz) Wavelength: The length from the one crest of a wave to the next. I. Electromagnetic

More information

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9 Module 9 This module presents information on what X-rays are and how they are produced. Introduction Module 9, Page 2 X-rays are a type of electromagnetic radiation. Other types of electromagnetic radiation

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

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

Name: COMBINED SCIENCE Topics 4, 5 & 6 LEARNING OUTCOMES. Maintain a record of your progress Use the booklet to guide revision

Name: COMBINED SCIENCE Topics 4, 5 & 6 LEARNING OUTCOMES. Maintain a record of your progress Use the booklet to guide revision Name: COMBINED SCIENCE Topics 4, 5 & 6 LEARNING OUTCOMES Maintain a record of your progress Use the booklet to guide revision Close the Gap Contemporary record of the Topics / Learning outcomes that I

More information

Chapter 38. Photons Light Waves Behaving as Particles

Chapter 38. Photons Light Waves Behaving as Particles Chapter 38 Photons Light Waves Behaving as Particles 38.1 The Photoelectric Effect The photoelectric effect was first discovered by Hertz in 1887, and was explained by Einstein in 1905. The photoelectric

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

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

Analytical Methods for Materials

Analytical Methods for Materials Analytical Methods for Materials Lesson 6 Production & Properties of X-rays Suggested Reading Chapter 1 in Waseda et al. Section 2.1 in Leng Other Reference B.D. Cullity and S.R. Stock, Elements of X-ray

More information

1-D Fourier Transform Pairs

1-D Fourier Transform Pairs 1-D Fourier Transform Pairs The concept of the PSF is most easily explained by considering a very small point source being placed in the imaging field-of-view The relationship between the image, I, and

More information

Radiation Response and Removals: Getting Down to the Nitty Gritty. 15 th Annual OSC Readiness Training Program

Radiation Response and Removals: Getting Down to the Nitty Gritty. 15 th Annual OSC Readiness Training Program Radiation Response and Removals: Getting Down to the Nitty Gritty 15 th Annual OSC Readiness Training Program www.oscreadiness.org 0 Radiation Fundamentals Tony Honnellio Health Physicist U.S. EPA, Region

More information

3 Radioactivity - Spontaneous Nuclear Processes

3 Radioactivity - Spontaneous Nuclear Processes 3 Radioactivity - Spontaneous Nuclear Processes Becquerel was the first to detect radioactivity. In 1896 he was carrying out experiments with fluorescent salts (which contained uranium) and found that

More information

10.1 RADIOACTIVE DECAY

10.1 RADIOACTIVE DECAY 10.1 RADIOACTIVE DECAY When Henri Becquerel placed uranium salts on a photographic plate and then developed the plate, he found a foggy image. The image was caused by rays that had not been observed before.

More information

Chapter 10. Table of Contents. Section 1 What Is Radioactivity? Section 2 Nuclear Fission and Fusion. Section 3 Nuclear Radiation Today

Chapter 10. Table of Contents. Section 1 What Is Radioactivity? Section 2 Nuclear Fission and Fusion. Section 3 Nuclear Radiation Today Nuclear Chemistry Table of Contents Section 1 What Is Radioactivity? Section 2 Nuclear Fission and Fusion Section 3 Nuclear Radiation Today Section 1 What Is Radioactivity? Bellringer Before studying about

More information

What happens during nuclear decay? During nuclear decay, atoms of one element can change into atoms of a different element altogether.

What happens during nuclear decay? During nuclear decay, atoms of one element can change into atoms of a different element altogether. When Henri Becquerel placed uranium salts on a photographic plate and then developed the plate, he found a foggy image. The image was caused by rays that had not been observed before. For his discovery

More information

Slide 1. Slide 2. Slide 3. Take the Terror Out of Physics. Active and Interactive Games and Activities for Teaching Radiographic Physics

Slide 1. Slide 2. Slide 3. Take the Terror Out of Physics. Active and Interactive Games and Activities for Teaching Radiographic Physics Slide 1 Active and Interactive Games and Activities for Teaching Radiographic Physics Jennifer Yates, MS, RT(R)(M)(BD) AEIRS 2010 Slide 2 Take the Terror Out of Physics X-Ray Tube Bingo Game Immediate

More information

DR KAZI SAZZAD MANIR

DR KAZI SAZZAD MANIR DR KAZI SAZZAD MANIR PHOTON BEAM MATTER ENERGY TRANSFER IONISATION EXCITATION ATTENUATION removal of photons from the beam by the matter. ABSORPTION SCATTERING TRANSMISSION Taking up the energy from the

More information

3. The very long ones are called waves, and the very short ones are called waves.

3. The very long ones are called waves, and the very short ones are called waves. NASA Mission: Science Introduction to the Electromagnetic Spectrum Web Quest Directions: Load the following website which will discuss the electromagnetic spectrum in detail. http://missionscience.nasa.gov/ems/01_intro.html

More information

Interaction of Ionizing Radiation with Matter

Interaction of Ionizing Radiation with Matter Type of radiation charged particles photonen neutronen Uncharged particles Charged particles electrons (β - ) He 2+ (α), H + (p) D + (d) Recoil nuclides Fission fragments Interaction of ionizing radiation

More information

For the next several lectures, we will be looking at specific photon interactions with matter. In today s lecture, we begin with the photoelectric

For the next several lectures, we will be looking at specific photon interactions with matter. In today s lecture, we begin with the photoelectric For the next several lectures, we will be looking at specific photon interactions with matter. In today s lecture, we begin with the photoelectric effect. 1 The objectives of today s lecture are to identify

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

10/27/2017 [pgs ]

10/27/2017 [pgs ] Objectives SWBAT explain the relationship between energy and frequency. SWBAT predict the behavior of and/or calculate quantum and photon energy from frequency. SWBAT explain how the quantization of energy

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

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

1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level)

1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level) 1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level) Electromagnetic induction (Chapter 23): For a straight wire, the induced current or e.m.f. depends on: The magnitude of the magnetic

More information

At the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation.

At the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation. RADIOACTIVITY - SPONTANEOUS NUCLEAR PROCESSES OBJECTIVES At the conclusion of this lesson the trainee will be able to: 1. For~, p and 7 decays a) Write a typical equation for the production of each type

More information

Warm-up Which of the following is NOT made up of photons?

Warm-up Which of the following is NOT made up of photons? Warm-up Which of the following is NOT made up of photons? 1. Laser light 2. Radio waves 3. Ultrasonic waves 4. X-rays Radio µwaves fir IR uv x-ray gamma-ray... Xrays Discovered by Wm. Roentgen in 1895

More information

CHAPTER 2 INTERACTION OF RADIATION WITH MATTER

CHAPTER 2 INTERACTION OF RADIATION WITH MATTER CHAPTER 2 INTERACTION OF RADIATION WITH MATTER 2.1 Introduction When gamma radiation interacts with material, some of the radiation will be absorbed by the material. There are five mechanisms involve in

More information

X-RAY SPECTRA. Theory:

X-RAY SPECTRA. Theory: 12 Oct 18 X-ray.1 X-RAY SPECTRA In this experiment, a number of measurements involving x-rays will be made. The spectrum of x-rays emitted from a molybdenum target will be measured, and the experimental

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 4 - Detectors Binding Energy Nuclear mass MN less than sum of nucleon masses Shows nucleus is a bound (lower energy) state for this configuration

More information

SECTION A Quantum Physics and Atom Models

SECTION A Quantum Physics and Atom Models AP Physics Multiple Choice Practice Modern Physics SECTION A Quantum Physics and Atom Models 1. Light of a single frequency falls on a photoelectric material but no electrons are emitted. Electrons may

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

Section 3: Nuclear Radiation Today

Section 3: Nuclear Radiation Today : Nuclear Radiation Today Preview Key Ideas Bellringer Where is Radiation? Beneficial Uses of Nuclear Radiation Risks of Nuclear Radiation Nuclear Power Key Ideas Where are we exposed to radiation? What

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

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

Ch4 and Ch5. Atomic History and the Atom

Ch4 and Ch5. Atomic History and the Atom Ch4 and Ch5 Atomic History and the Atom Ch4.2 What are atoms? Atoms are the smallest part of an element that still has the element s properties. Ch. 4.3 The Atom is Defined 400 B.C. the Greek philosopher

More information

EDS User School. Principles of Electron Beam Microanalysis

EDS User School. Principles of Electron Beam Microanalysis EDS User School Principles of Electron Beam Microanalysis Outline 1.) Beam-specimen interactions 2.) EDS spectra: Origin of Bremsstrahlung and characteristic peaks 3.) Moseley s law 4.) Characteristic

More information

Radiation Safety. PIXE PAN 2008 Ed Stech University of Notre Dame

Radiation Safety. PIXE PAN 2008 Ed Stech University of Notre Dame Radiation Safety PIXE PAN 2008 Ed Stech University of Notre Dame Outline Radiation Overview Radiation Safety in during PIXE PAN Other Safety Issues Ionizing Radiation 4 Types Alpha Beta Photon (Gamma and

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

X-ray Spectroscopy. Danny Bennett and Maeve Madigan. October 12, 2015

X-ray Spectroscopy. Danny Bennett and Maeve Madigan. October 12, 2015 X-ray Spectroscopy Danny Bennett and Maeve Madigan October 12, 2015 Abstract Various X-ray spectra were obtained, and their properties were investigated. The characteristic peaks were identified for a

More information

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

Physics 102: Lecture 26. X-rays. Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1 Physics 102: Lecture 26 X-rays Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1 X-Rays Photons with energy in approx range 100eV to 100,000eV. This large energy means they

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

PHYS 3650L - Modern Physics Laboratory

PHYS 3650L - Modern Physics Laboratory PHYS 3650L - Modern Physics Laboratory Laboratory Advanced Sheet Photon Attenuation 1. Objectives. The objectives of this laboratory exercise are: a. To measure the mass attenuation coefficient at a gamma

More information

Rb, which had been compressed to a density of 1013

Rb, which had been compressed to a density of 1013 Modern Physics Study Questions for the Spring 2018 Departmental Exam December 3, 2017 1. An electron is initially at rest in a uniform electric field E in the negative y direction and a uniform magnetic

More information

Introduction to Ionizing Radiation

Introduction to Ionizing Radiation Introduction to Ionizing Radiation Bob Curtis OSHA Salt Lake Technical Center Supplement to Lecture Outline V. 10.02 Basic Model of a Neutral Atom Electrons(-) orbiting nucleus of protons(+) and neutrons.

More information

Chapter NP-4. Nuclear Physics. Particle Behavior/ Gamma Interactions TABLE OF CONTENTS INTRODUCTION OBJECTIVES 1.0 IONIZATION

Chapter NP-4. Nuclear Physics. Particle Behavior/ Gamma Interactions TABLE OF CONTENTS INTRODUCTION OBJECTIVES 1.0 IONIZATION Chapter NP-4 Nuclear Physics Particle Behavior/ Gamma Interactions TABLE OF CONTENTS INTRODUCTION OBJECTIVES 1.0 IONIZATION 2.0 ALPHA PARTICLE INTERACTIONS 3.0 BETA INTERACTIONS 4.0 GAMMA INTERACTIONS

More information

Detecting high energy photons. Interactions of photons with matter Properties of detectors (with examples)

Detecting high energy photons. Interactions of photons with matter Properties of detectors (with examples) Detecting high energy photons Interactions of photons with matter Properties of detectors (with examples) Interactions of high energy photons with matter Cross section/attenution length/optical depth Photoelectric

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 17, Electromagnetic Waves Physical Science, McDougal-Littell, 2008

Chapter 17, Electromagnetic Waves Physical Science, McDougal-Littell, 2008 SECTION 1 (PP. 553-558): ELECTROMAGNETIC WAVES HAVE UNIQUE TRAITS. Georgia Standards: S8P4a Identify the characteristics of electromagnetic and mechanical waves; S8P4d Describe how the behavior of waves

More information

X-ray Energy Spectroscopy (XES).

X-ray Energy Spectroscopy (XES). X-ray Energy Spectroscopy (XES). X-ray fluorescence as an analytical tool for element analysis is based on 3 fundamental parameters: A. Specificity: In determining an x-ray emission energy E certainty

More information

((Radiation )) أيهمدغيم. Ionizing RadiationNon-ionizing radiation. This is the last sheet for Dr. Madi s lectures & its number is ((22)).

((Radiation )) أيهمدغيم. Ionizing RadiationNon-ionizing radiation. This is the last sheet for Dr. Madi s lectures & its number is ((22)). ((Radiation )) This is the last sheet for Dr. Madi s lectures & its number is ((22)). This sheet contains (Slides and recording).. So I did my best to let you not refer to slides. First of all, there is

More information

NAT 5 - Waves and Radiation Powerpoint Answers

NAT 5 - Waves and Radiation Powerpoint Answers NAT 5 - Waves and Radiation Powerpoint Answers 1. Light is a form of energy. 2. Angle of incidence = 60º. Angle of reflection = 60º. 3. Refraction is the change in the speed of light when moving from one

More information

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

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? 2. Briefly discuss dead time in a detector. What factors are important

More information

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7 Advanced Lab Course X-Ray Photoelectron Spectroscopy M210 As of: 2015-04-01 Aim: Chemical analysis of surfaces. Content 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT 3 3.1 Qualitative analysis 6 3.2 Chemical

More information

Chapter 30 X Rays GOALS. When you have mastered the material in this chapter, you will be able to:

Chapter 30 X Rays GOALS. When you have mastered the material in this chapter, you will be able to: Chapter 30 X Rays GOALS When you have mastered the material in this chapter, you will be able to: Definitions Define each of the following terms, and use it in an operational definition: hard and soft

More information

Radiation Safety for X-ray Diffraction

Radiation Safety for X-ray Diffraction Radiation Safety for X-ray Diffraction Overview of Issue: Exposure types Short-term high-dose Long-term low-dose Invisible, odorless colorless; most exposures undetectable Lab users must understand radiation

More information

CHAPTER 3 The Experimental Basis of Quantum Theory

CHAPTER 3 The Experimental Basis of Quantum Theory CHAPTER 3 The Experimental Basis of Quantum Theory 3.1 3.2 3.3 3.4 3.5 3.6 3.7 3.8 3.9 Discovery of the X Ray and the Electron Determination of Electron Charge Line Spectra Quantization As far as I can

More information

UNCORRECTED PROOF. Table of Contents

UNCORRECTED PROOF. Table of Contents 00-Stabin-Prelims SNY001-Stabin (Typeset by spi publisher services, Delhi) vii of xvi June 1, 2007 17:15 Preface xiii Acknowledgments xv Chapter 1. Introduction to Health Physics 1 1.1 Definition of Health

More information

Interaction theory Photons. Eirik Malinen

Interaction theory Photons. Eirik Malinen Interaction theory Photons Eirik Malinen Introduction Interaction theory Dosimetry Radiation source Ionizing radiation Atoms Ionizing radiation Matter - Photons - Charged particles - Neutrons Ionizing

More information

Physics 3204 UNIT 3 Test Matter Energy Interface

Physics 3204 UNIT 3 Test Matter Energy Interface Physics 3204 UNIT 3 Test Matter Energy Interface 2005 2006 Time: 60 minutes Total Value: 33 Marks Formulae and Constants v = f λ E = hf h f = E k + W 0 E = m c 2 p = h λ 1 A= A T 0 2 t 1 2 E k = ½ mv 2

More information

Units and Definition

Units and Definition RADIATION SOURCES Units and Definition Activity (Radioactivity) Definition Activity: Rate of decay (transformation or disintegration) is described by its activity Activity = number of atoms that decay

More information

Chapter 4 - Light. Name: Block:

Chapter 4 - Light. Name: Block: Chapter 4 Notes: Light Name: Block: Properties of Waves Waves are a repeating disturbance or movement that energy through matter or space without causing any displacement of material Features of a wave:

More information

Honors Ch3 and Ch4. Atomic History and the Atom

Honors Ch3 and Ch4. Atomic History and the Atom Honors Ch3 and Ch4 Atomic History and the Atom Ch. 3.1 The Atom is Defined 400 B.C. the Greek philosopher Democritus said that the world was made of two things: Empty space and tiny particles called atoms

More information

1 The Cathode Rays experiment is associated. with: Millikan A B. Thomson. Townsend. Plank Compton

1 The Cathode Rays experiment is associated. with: Millikan A B. Thomson. Townsend. Plank Compton 1 The Cathode Rays experiment is associated with: A B C D E Millikan Thomson Townsend Plank Compton 1 2 The electron charge was measured the first time in: A B C D E Cathode ray experiment Photoelectric

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