How Things Work II. (Lecture #32) Instructor: Gordon D. Cates Office: Physics 106a, Phone: (434)

Similar documents
Energy. on this world and elsewhere. Instructor: Gordon D. Cates Office: Physics 106a, Phone: (434)

Physics of Nuclear Weapons

Energy. on this world and elsewhere. Instructor: Gordon D. Cates Office: Physics 106a, Phone: (434)

Appendix A. Physics and Technology of Nuclear-Explosive Materials

Energy. on this world and elsewhere. Visiting today: Prof. Paschke

NOTES: 25.3 Nuclear Fission & Fusion

Radioactivity. L 38 Modern Physics [4] Hazards of radiation. Nuclear Reactions and E = mc 2 Einstein: a little mass goes a long way

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

Nuclear Chemistry. Chapter 24

One nucleus splits into two smaller nuclei and typically a few neutrons by the bombardment of a neutron. U-235 is the only naturally occurring

Chemistry 500: Chemistry in Modern Living. Topic 5: The Fires of Nuclear Fission. Atomic Structure, Nuclear Fission and Fusion, and Nuclear.

Step 2: Calculate the total amount of U-238 present at time=0. Step 4: Calculate the rate constant for the decay process.

Term 3 Week 2 Nuclear Fusion & Nuclear Fission

Relative abundances of carbon isotopes in our atmosphere are:

4.4 Atomic structure Notes

Unpressurized steam reactor. Controlled Fission Reactors. The Moderator. Global energy production 2000

L 36 Modern Physics :006 FINAL EXAM. Nuclear reactions: E = mc 2. Radioactivity. Hazards of radiation. Biological effects of nuclear radiation

Nuclear Reactions and E = mc 2. L 38 Modern Physics [4] Hazards of radiation. Radiation sickness. Biological effects of nuclear radiation

Unit 2: Atomic Theory Notes

Physics 11 Nuclear Process. Nuclear Fusion Reactors Terminology Waste Storage Radiation and living things Nuclear Fission

L 36 Atomic and Nuclear Physics-4. Radioactivity. Nuclear reactions: E = mc 2. Hazards of radiation. Biological effects of nuclear radiation

Nuclear Chemistry. Background Radiation. Three-fourths of all exposure to radiation comes from background radiation.

WELCOME TO PERIOD 18: CONSEQUENCES OF NUCLEAR ENERGY

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

nuclear chemical change CH4 + 2O2 CO2 + 2H2O carbon dating

Carbon Dating. Principles of Radiometric Dating. 03 nuclear decay and the standard model June 05, 2013

Nuclear processes: Vocabulary: Radioactive decay Isotope Alpha particle Beta particle Transmutation Strong Nuclear Force Fusion fission

Chapter 17. Radioactivity and Nuclear Chemistry

Nuclear Fission. Conceptual Physics 11 th Edition. Nuclear Fission. Nuclear Fission. Nuclear Fission. This lecture will help you understand:

Isotopes. An isotope is an atom of the same element (same number of protons) that varies in the number of neutrons.

Isotopes. An isotope is an atoms of the same element (same number of protons) that vary in the number of neutrons.

The Physics of Nuclear Reactors. Heather King Physics 420

Scottish CND - Education Pack

Science 10 Radioactivity Review v3

Nuclear Chemistry Unit

The discovery of nuclear reactions need not bring about the destruction of mankind any more than the discovery of matches - Albert Einstein

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

nuclear fission nucleus slightly mass

Physics/Global Studies 280 Nuclear Weapons, Nuclear War, and Arms Control. Midterm Examination March 15

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

Nuclear processes: Vocabulary: Radioactive decay Isotope Alpha particle Beta particle Transmutation Strong Nuclear Force Fusion Fission

Nuclear power plants can generate large amounts of electricity.

Isotopes Atoms of an element (same # p+) that differ in their number of neutrons

11.5 Nuclear Reactions: Fusion

Phys 1020 Day 27 Finish nuclear energy Radiation and Nuclear Reactors, Blmfd 16.2 Exponential Growth Energy Use

Nuclear Fission & Fusion

Name Chemistry-PAP Per. Notes: Atomic Structure

2 Energy from the Nucleus

PHYS:1200 LECTURE 36 ATOMIC AND NUCLEAR PHYSICS (4)

Production. David Nusbaum Project on Managing the Atom, Belfer Center October 4, 2011

Chapter 21 - Nuclear Chemistry Applications

21/11/ /11/2017 Atomic Structure AQA Physics topic 4

Nuclear fission and fusion are processes that involve extremely large amounts of energy.

Nonrenewable Energy: Nuclear. Energy Part 2

Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

Energy. on this world and elsewhere. Instructor: Gordon D. Cates Office: Physics 106a, Phone: (434)

Unit 3: Chemistry in Society Nuclear Chemistry Summary Notes

Chapter 10. Section 10.1 What is Radioactivity?

Energy & Sustainability

Lecture Presentation. Chapter 21. Nuclear Chemistry. James F. Kirby Quinnipiac University Hamden, CT Pearson Education, Inc.

NUCLEAR ENERGY! DAY 1: (RADIATION, FISSION, FUSION)

c) O-16 d) Pu An unstable nucleus emits. a) Atoms b) Electricity c) Plasma d) Radiation 3. Many of uranium are radioactive. a) Ions b) Isomers

UNIT 10 RADIOACTIVITY AND NUCLEAR CHEMISTRY

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

40 Nuclear Fission and Fusion. Nuclear fission and nuclear fusion reactions release huge amounts of energy.

6 Neutrons and Neutron Interactions

Nuclear Chemistry. Transmutations and the Creation of Elements

Lecture 14, 8/9/2017. Nuclear Reactions and the Transmutation of Elements Nuclear Fission; Nuclear Reactors Nuclear Fusion

General Physics (PHY 2140)

Lecture 7 Problem Set-2

A is called the mass number gives, roughly, the mass of the nucleus or atom in atomic mass units = amu = u

Mass number i. Example U (uranium 235) and U (uranium 238) atomic number e. Average atomic mass weighted of the isotopes of that element i.

What do the nuclei of different molybdenum isotopes have in common?

Nuclear Reactions. page 1

UNIT 10 RADIOACTIVITY AND NUCLEAR CHEMISTRY

10.4 Fission and Fusion

Ch 17 Radioactivity & Nuc. Chemistry Study Guide Accelerated Chemistry SCANTRON

Nuclear Weapons (and Energy)

Science 10: Radioactivity! Comparing Fission and Fusion Notes (Ch 11)

Notes: Part 1 - Nuclear Chemistry

Chapter 18. Nuclear Chemistry

Thinking Like a Chemist About Nuclear Change!

A Nuclear Power Plant

Lecture PowerPoint. Chapter 31 Physics: Principles with Applications, 6 th edition Giancoli

Nuclear Chemistry CHAPTER

Nuclear Chemistry AP Chemistry Lecture Outline

Chapter 10 Section 4 Notes

Physics 180. Nuclear Weapons, Nuclear War, and Arms Control

2. Electrons: e - charge = negative -1 mass ~ 0

Wallace Hall Academy Physics Department. Radiation. Pupil Notes Name:

NUCLEI. Atomic mass unit

UNIT 13: NUCLEAR CHEMISTRY

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

Atomic & Nuclear Physics

Nuclear Chemistry. Nuclear Terminology

By Tim, John, Shane, Owen

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

Alpha Decay Simulation

Nuclear Energy Fundamentals

RADIOACTIVITY & HALF-LIFE Part 3

Transcription:

How Things Work II (Lecture #32) Instructor: Gordon D. Cates Office: Physics 106a, Phone: (434) 924-4792 email: cates@virginia.edu Course web site available through COD and Toolkit or at http://people.virginia.edu/~gdc4k/phys106/spring08 April 11, 2008

Announcements Final exam will be Thursday, May 1st, from 9-12AM. Please read Chapter 16 in your text. Problem Set #5 will be posted within the next few days.

Question On average, in order to sustain a chain reaction, how many neutrons must be captured by U-235 nuclei following the fission of a single U-235 nucleus? A. 0. B. more than 1 C. more than 1.5 D. more than 2.0 E. more than 3.0

Not all uranium is the same! This is the stuff out of which you can make bombs and reactors. 238 92 U 235 92 U 99.27% of all uranium is U-238 When hit by a neutron it will sometimes undergo fission, but most of the time the neutron is just absorbed. 0.63% of all uranium is U-235 When hit by a neutron it will almost always undergo fission. Both U-238 and U235 are unstable, but U-235 is more unstable than U-238 (half-lives of 4.5x10 9 and 7.0x10 8 years respectively). This is why most of the naturally occurring uranium is U-238.

It is very difficult to separate the two isotopes of uranium 238 92 U 99.27% 235 92 U 0.63% Chemically they are essentially identical. You can only separate them by taking advantage of the fact that their masses are different.

Secret efforts to develop the bomb Article from NY Times the day after the bombing of Hiroshima (August 7th, 1945) describing the hidden cities where the materials to make the bombs, and the bombs themselves, were produced.

The simplest atom bomb - using U-235 If a sphere of U-235 is big enough, on average, more than one neutron per fission reaction will cause another fission reaction. This happens with a sphere of roughly 52 kg, around 17 cm in diameter. The simplest nuclear weapon simply assembles this critical mass. Not shown is the trigger that releases neutrons at the key moment.

Video of bomb tests and results

Little Boy - dropped on Hiroshima Photos and text from U.S. Dept. of Energy website. No one will ever know for certain how many died as a result of the attack on Hiroshima. Some 70,000 people probably died as a result of initial blast, heat, and radiation effects. This included about twenty American airmen being held as prisoners in the city. By the end of 1945, because of the lingering effects of radioactive fallout and other after effects, the Hiroshima death toll was probably over 100,000. The five-year death total may have reached or even exceeded 200,000, as cancer and other long-term effects took hold.

Little Boy - dropped on Hiroshima Though already eleven and a half miles away, the Enola Gay was rocked by the blast. At first, Tibbets [Captain and pilot of the Enola Gay] thought he was taking flak. After a second shock wave (reflected from the ground) hit the plane, the crew looked back at Hiroshima. "The city was hidden by that awful cloud... boiling up, mushrooming, terrible and incredibly tall," Tibbets recalled. The yield of the explosion was later estimated at 15 kilotons (the equivalent of 15,000 tons of TNT).

Plutonium-239, the other commonly used material for making nuclear weapons Plutonium is different from U-235 in that it undergoes spontaneous fission much more often than does U-235 (by a factor of just over 100). Consequently, a cannon-like design would result in a core that would blow itself apart before undergoing an efficient explosion.

Plutonium-based weapons With 239 Pu a cannon-like design would result would blow apart prematurely, resulting in an efficient explosion. For this reason, and implosion-based design was developed.

Cross-section view of Fat Man This is the design that was tested near Alamogordo, New Mexico, on June 16, 1945. The critical mass for Pu-239 is around 10 kg, but Fat Man used a subcritical mass of around 6.1 kg, which was sufficient after being compressed by the implosion.

Fat Man - dropped on Nagasaki The explosion affected a total area of approximately 43 square miles. According to a Nagasaki Prefectural report "men and animals died almost instantly" within 1 kilometer (0.62 miles) of the point of detonation. Almost all homes within a mile and a half were destroyed, and dry, combustible materials such as paper instantly burst into flames as far away as 10,000 feet from ground zero. Of the 52,000 homes in Nagasaki, 14,000 were destroyed and 5,400 more seriously damaged. Only 12 percent of the homes escaped unscathed. As with the estimates of deaths at Hiroshima, it will never be known for certain how many people died as a result of the atomic attack on Nagasaki. The best estimate is 40,000 people died initially, with 60,000 more injured. By January 1946, the number of deaths probably approached 70,000, with perhaps ultimately twice that number dead total within five years.

Video of bomb tests and results

The Davy Crockett

The Davy Crockett

Plutonium can be manufactured in a nuclear reactor Breeding plutonium from U-238 When U-238 captures a neutron, after two beta decays, it turns into Pu-239, the fissionable isotope of plutonium. Thus, fuel rods in a nuclear reactor will, after time, contain 239 Pu. Plutonium is chemically different from uranium and can be extracted chemically. The reprocessing of the fuel rods to extract plutonium is complicated and difficult, but far easier than isotopic separation.

Proliferation Issues 235 U - Requires isotopic separation. Major industrial effort. 239 Pu - Can be obtained from re-processed fuel rods, which of course implies you already have nuclear reactors.