Radioactivity. Nuclear Physics. # neutrons vs# protons Where does the energy released in the nuclear 11/29/2010 A=N+Z. Nuclear Binding, Radioactivity

Similar documents
Nuclear Physics. Radioactivity. # protons = # neutrons. Strong Nuclear Force. Checkpoint 4/17/2013. A Z Nucleus = Protons+ Neutrons

Nuclear Binding, Radioactivity

Nuclear Binding, Radioactivity

Nuclear Binding, Radioactivity

Physics 102: Lecture 28

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

Phys 102 Lecture 27 The strong & weak nuclear forces

Thursday, April 23, 15. Nuclear Physics

Basic Nuclear Theory. Lecture 1 The Atom and Nuclear Stability

H 1. Nuclear Physics. Nuclear Physics. 1. Parts of Atom. A. Nuclear Structure. 2b. Nomenclature. 2. Isotopes. AstroPhysics Notes

H 1. Nuclear Physics. Nuclear Physics. 1. Parts of Atom. 2. Isotopes. AstroPhysics Notes. Dr. Bill Pezzaglia. Rough draft. A.

Chemistry 52 Chapter 11 ATOMIC STRUCTURE. The general designation for an atom is shown below:

The strong & weak nuclear forces

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

Chapter 22 - Nuclear Chemistry

Alta Chemistry CHAPTER 25. Nuclear Chemistry: Radiation, Radioactivity & its Applications

Chem 481 Lecture Material 1/23/09

General Physics (PHY 2140)

Nuclear Physics and Nuclear Reactions

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

Sources of Radiation

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

da u g ht er + radiation

Chapter 22. Preview. Objectives Properties of the Nucleus Nuclear Stability Binding Energy Sample Problem. Section 1 The Nucleus

Chapter 12: Nuclear Reaction

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

A. Incorrect! Do not confuse Nucleus, Neutron and Nucleon. B. Incorrect! Nucleon is the name given to the two particles that make up the nucleus.

NUCLEI, RADIOACTIVITY AND NUCLEAR REACTIONS

Introduction to Nuclear Reactor Physics

Chapter 25. Nuclear Chemistry. Types of Radiation

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of?

Nuclear Physics and Radioactivity

: When electrons bombarded surface of certain materials, invisible rays were emitted

Journal 14. What is so dangerous about nuclear energy?


ABC Math Student Copy

Nuclear Powe. Bronze Buddha at Hiroshima

Particles involved proton neutron electron positron gamma ray 1

Physics 11. Unit 10 Nuclear Physics

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

Nuclear Chemistry Notes

Unit 1 Atomic Structure

Nuclear Chemistry. Mass Defect. E=mc 2. Radioactivity. Types of Radiation. Other Nuclear Particles. Nuclear Reactions vs. Normal Chemical Changes

Chemistry 201: General Chemistry II - Lecture

Phys102 Lecture 29, 30, 31 Nuclear Physics and Radioactivity

LECTURE 23 NUCLEI. Instructor: Kazumi Tolich

NUCLEI. Atomic mass unit

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]

Chemistry 1000 Lecture 3: Nuclear stability. Marc R. Roussel

Chemistry: The Central Science. Chapter 21: Nuclear Chemistry

Revision Guide for Chapter 18

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

Chapter 3. Radioactivity. Table of Contents

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

General Physics (PHY 2140)

Chapter 19 - Nuclear Chemistry Nuclear Stability and Modes of Decay

Unit 1 Atomic Structure

Chapter. Nuclear Chemistry

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

Unit 6 Nuclear Radiation Parent Guide. What is radioactivity and why are things radioactive?

LECTURE 25 NUCLEAR STRUCTURE AND STABILITY. Instructor: Kazumi Tolich

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

Preview. Subatomic Physics Section 1. Section 1 The Nucleus. Section 2 Nuclear Decay. Section 3 Nuclear Reactions. Section 4 Particle Physics

Chapter 20: Phenomena. Chapter 20: The Nucleus: A Chemist s View. Nuclear Decay. Nuclear Decay. Nuclear Decay. Nuclear Decay

Nuclear Reactions. Nuclear Reactions

Chapter 29. Nuclear Physics

Populating nucleon states. From the Last Time. Other(less stable) helium isotopes. Radioactivity. Radioactive nuclei. Stability of nuclei.

Nuclear Chemistry Lecture Notes: I Radioactive Decay A. Type of decay: See table. B. Predicting Atomic Stability

Conceptual Physics Nuclear Physics

Chapter 44. Nuclear Structure

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

Fission and Fusion Book pg cgrahamphysics.com 2016

SAVE PAPER AND INK!!!

Nuclear Spectroscopy: Radioactivity and Half Life

Physics 3204 UNIT 3 Test Matter Energy Interface

NJCTL.org 2015 AP Physics 2 Nuclear Physics

Radioactivity pp Topic 9: Nuclear Physics Ch. 10. Radioactivity. Radioactivity

= : K A

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

Nuclear Chemistry. Proposal: build a nuclear power plant in Broome County. List the pros & cons


THE NUCLEUS: A CHEMIST S VIEW Chapter 20

Chapter 28 Lecture. Nuclear Physics Pearson Education, Inc.

Unit 3: Chemistry in Society Nuclear Chemistry Summary Notes

THE NUCLEUS OF AN ATOM

Nuclear Reactions. Nuclear Reactions

6. Atomic and Nuclear Physics

Radioisotopes. alpha. Unstable isotope. stable. beta. gamma

Chapter 18 Nuclear Chemistry

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

Fiesta Ware. Nuclear Chemistry. 2009, Prentice-Hall, Inc.

Class XII Chapter 13 - Nuclei Physics

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

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

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

Nuclear Chemistry Review Packet

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.

Chapter 10 - Nuclear Physics

Nuclear 2. Fission and Fusion

CHAPTER 12 The Atomic Nucleus

Transcription:

Physics 1161: Lecture 25 Nuclear Binding, Radioactivity Sections 32-1 32-9 Marie Curie 1867-1934 Radioactivity Spontaneous emission of radiation from the nucleus of an unstable isotope. Antoine Henri Becquerel 1852-1908 Wilhelm Roentgen 1845-1923 A Z 6 3 Li Nuclear Physics Nucleus = Protons+ Neutrons nucleons Z = N = A material is known to be an isotope of lead. Which of the following can be specified? 1. The atomic mass number 2. The neutron number 3. The number of protons A = nucleon number (atomic mass number) Gives you mass density of element A=N+Z Periodic_Table # neutrons vs# protons Where does the energy released in the nuclear But protons repel one another (Coulomb Force) and when Z is large it becomes harder to put more protons into a nucleus without adding even more neutrons to provide more of the Strong Force. For this reason, in heavier nuclei N>Z. reactions of the sun come from? 1. covalent bonds between atoms 2. binding energy of electrons to the nucleus 3. binding energy of nucleons 1

Strong Nuclear Force Acts on Protons and Neutrons Strong enough to overcome Coulomb repulsion Acts over very short distances Two atoms don t feel force Strong Nuclear Force Hydrogen atom: Binding energy =13.6eV (of electron to nucleus) Coulomb force electron proton neutron Simplest Nucleus: Deuteron=neutron+proton Very strong force Binding energy ofdeuteron = 2.2 10 6 ev 2.2Mev! proton or Binding Energy Einstein s famous equation E = m c 2 Binding Energy Plot Iron (Fe) has the most binding energy/nucleon. Lighter have too few nucleons, heavier have too many. 10 Proton: mc 2 = 938.3MeV Neutron: mc 2 = 939.5MeV Deuteron: mc 2 =1875.6MeV Adding these, gives 1877.8MeV Difference is Binding energy, 2.2MeV M Deuteron = M Proton + M Neutron Binding Energy BINDING ENERGY in MeV/nucleon 238 92U Mass/Nucleon vs Atomic Number Fusion Fission E = mc 2 E: energy m: mass c: speed of light c = 3 x 10 8 m/s 2

E = mc 2 Mass can be converted to energy Energy can be converted to mass Mass and energy are the same thing Mass Defect in Fission When a heavy element (one beyond Fe) fissions, the resulting products have a combined mass which is less than that of the original nucleus. Mass Defect of Alpha Particle Mass difference = 0.0304 u Binding energy = 28.3 MeV Fusion product has less mass than the sum of the parts. Which of the following is most correct for the total binding energy of an Iron atom (Z=26)? 1. 9 MeV 2. 234 MeV 3. 270 MeV 4. 504 Mev BINDING ENERGY in MeV/nucleon 0% 0% 0% 0% 1 2 3 4 B field into screen 3 Types of Radioactivity Alpha Decay Radioactive sources α particles: 4 He nucleii 2 detector β particles: electrons γ: photons (more energetic than x-rays) Alpha decay occurs when there are too many protons in the nucleus which cause excessive electrostatic repulsion. An alpha particle is ejected from the nucleus. An alpha particle is 2 protons and 2 neutrons. An alpha particle is also a helium nucleus. Alpha particle symbol: 4 2 He 3

Beta Decay Beta decay occurs when neutron to proton ratio is too big A neutron is turned into a proton and electron and an antineutrino The electron and the antineutrino are emitted Gamma Decay Gamma decay occurs when the nucleus is at too high an energy Nucleus falls down to a lower energy level High energy photon gamma ray -is emitted α: example β: example Decay Rules 1) Nucleon Number is conserved. 2) Atomic Number (charge) is conserved. 3) Energy and momentum are conserved. 238 92U 234 90 Th+α A * A γ: example P P+ 0 Z Z 0γ recall 4 2He =α 1) 238 = 234 + 4 Nucleon number conserved 2) 92 = 90 + 2 Charge conserved 1 1 + 0 0 0n 1p 1e + 0 ν Needed to conserve energy and momentum. A nucleus undergoes αdecay. Which of the following is FALSE? 1. Nucleon number decreases by 4 2. Neutron number decreases by 2 3. Charge on nucleus increases by 2 The nucleus 234 undergoes β decay. Which 90Th of the following is true? 1. The number of protons in the daughter nucleus increases by one. 2. The number of neutrons in the daughter nucleus increases by one. 238 92 U Radioactive Decay 234 90 Th 234 91 Pa 4

U 238 Decay Decay Series Nuclear Decay Links http://physics.bu.edu/cc104/uudecay.html http://www.physics.umd.edu/lecdem/honr22 8q/notes/U238scheme.gif http://www.physics.umd.edu/lecdem/honr22 8q/notes/fourdecschemes.gif Which of the following decays is NOT allowed? 1. 2. 3. 4. 238 92U 234 90 Th+α 210 4 84 Po 82Pb+ 2He 214 14 C 14 6 7 N+γ 40 0 0 K + + ν 40 19 20p e 1 0 Decays per second, or activity : If the number of radioactive nuclei present is cut in half, how does the activity change? 1. It remains the same 2. It is cut in half 3. It doubles N t = λn No. of nuclei present decay constant Decays per second, or activity Start with 16 14 C atoms. N t = λn decay constant After 6000 years, there are only 8 left. How many will be left after another 6000 years? 1. 0 2. 4 3. 6 No. of nuclei present Decay Function N(t)= N 0 e λt t T = N 0 2 1/2 Every 6000 years ½ of atoms decay time 5

Radioactivity Quantitatively Decays per second, or activity Survival: No. of nuclei present at time t Instead of baseewe can use base2: e λt t = 2 Then we can write N t = λn decay constant N(t )= N 0 e λt No. we started with at t=0 T 1/2 where T1/2 = 0.693 λ Half life No. of nuclei present N(t )= N 0 e λt t T = N 0 2 1/2 Carbon Dating Cosmic rays cause transmutation of Nitrogen to Carbon-14 n+ N H+ C 1 14 1 14 0 7 1 6 C-14 is radioactive with a half-life of 5730 years It decays back to Nitrogen by beta decay C e+ N 14 0 14 6 1 7 The ratio of C-12 (stable) atoms to C-14 atoms in our atmosphere is fairly constant about 10 12 /1 This ratio is the same in living things that obtain their carbon from the atmosphere You are radioactive! One in 8.3x10 11 carbon atoms is 14 C which β decays with a ½ life of 5730 years. Determine # of decays/gram of Carbon. N 1.0 mole 12 g 1 8.3 10 23 ( 6.02 10 ) 14 = 11 λ =.693 T 1/ 2 = 6 10 10 atoms g Carbon Dating We just determined that living organisms should have a decay rate of about 0.23 decays/ gram of carbon. The bones of an ice man are found to have a decay rate of 0.115 decays/gram. We can estimate he died about 6000 years ago. N t = λn Summary Nuclear Reactions Nucleon number conserved Charge conserved Energy/Momentum conserved α particles = 4 nuclei 2He β - particles = electrons γ particles = high-energy photons Mass/Nucleon vs Atomic Number Fusion Fusion Fission Fission Survival: N(t)= N 0 e λt T 1/2 = 0.693 λ Decays Half-Life is time for ½ of atoms to decay 6

U-235 -- Fissile Abundance of U-235 U-235 Fission by Neutron Bombardment Possible U-235 Fission Chain Reaction Breeder Reaction 7

Breeder Reactor Small amounts of Pu-239 combined with U- 238 Fission of Pufrees neutrons These neutrons bombard U-238 and produce more Pu-239 in addition to energy 8