Fall 2010 PHYS 172: Modern Mechanics Lecture 11 – The Energy Principle Chapter 6.15 – 6.17, 7.1 – 7.2 ANNOUNCEMENT The Final Exam in Phys 172H is scheduled.

Slides:



Advertisements
Similar presentations
Radioactivity.
Advertisements

Review Draw a model of each of the hydrogen isotopes Hydrogen-1
20th Century Discoveries
7: Atomic and Nuclear Physics 7.3 Nuclear reactions, fission and fusion.
Fundamental Forces of the Universe
Chapter 29 Nuclear Physics.
Nuclear Physics Lesson 13
Nuclear Binding, Radioactivity Sections 32-1 – 32-9 Physics 1161: Lecture 33.
Nuclear Binding Energy
Board Work 1.What is the electrical interaction between a.a proton and another proton in a nucleus? b.a proton and a neutron in a nucleus? c.a neutron.
Section 2Nuclear Changes Nuclear Forces 〉 What holds the nuclei of atoms together? 〉 The stability of a nucleus depends on the nuclear forces that hold.
Chapter 10 Nuclear Physics. Copyright © Houghton Mifflin Company 10-2 Section 10.1: Symbols of the Elements An element is the fundamental atom by which.
The equation E = mc 2 is probably the most recognized symbol of physics. This equation tells us that matter and energy are really two forms of the same.
CHEMISTRY 1000 Topic #4: Nuclear Chemistry Fall 2010 Dr. Susan Lait.
Welcome to Physics 7C! Lecture 8 -- Winter Quarter Professor Robin Erbacher 343 Phy/Geo
Nuclear Fission and Fusion
Slide 1 Test 2 results Test 2 average: 77 (test 1: 82) Test 2 median: 79 (test 1: 87)
Center of Mass. Motion of the Center of Mass The center of mass of a system moves as if all of the mass of the system were concentrated at that point.
Nuclear Physics Selected Topics 5 –Fission and Fusion.
Momentum For N particles: Why bother introducing one more definition? Most general form of the Newton’s law: Valid when mass is changing Valid in relativistic.
Radioactivity – types of decays presentation for April 28, 2008 by Dr. Brian Davies, WIU Physics Dept.
A nucleus is more than just mass
Nuclear Force and Particles
Learning Targets I can name the force that holds the atom’s nucleus together I can describe the two reasons why some isotopes are radioactive. I can describe.
Nuclear Physics Physics 12. Protons, Neutrons and Electrons  The atom is composed of three subatomic particles: Particle Charge (in C) Symbol Mass (in.
Matching the Content to Your Class (I was told there would be no math)
Modern Physics Radioactive Decay. Look at the periodic table given to you. Find element with the atomic number 6 What is it?
Unit 8 Section 2: Nuclear Reactions
PHYS 221 Recitation Kevin Ralphs Week 14. Overview Nuclear Physics – Structure of the Nucleus – Nuclear Reactions.
"More than any other time in history, mankind faces a crossroads. One path leads to despair and utter hopelessness. The other, to total extinction. Let.
Nuclear Chemistry.
Topic – Physics 2a Mass defect and binding energy Prior learning Atomic structure Electrical forces Key words –Atomic nucleus,mass difference, mass of.
Chapter 29 Nuclear Physics. Properties of Nuclei All nuclei are composed of protons and neutrons (exception: ordinary hydrogen) The atomic number, Z,
Lecture 1 & 2 © 2015 Calculate the mass defect and the binding energy per nucleon for a particular isotope.Calculate the mass defect and the binding.
Nuclear Reactions E = mc2
Protons and neutrons are called nucleons. An atom is referred to as a nuclide. An atom is identified by the number of protons and neutrons in its nucleus.
Nuclear Fusion By: Yours Truly, Christie Osadchy, and The Fool Who Ripped His Pants.
Nuclear Radiation 9.2. The Nucleus Protons and neutrons Charge of electrons and protons – x C = e –Proton +e –Electron -e.
Jeopardy $100 Fundamental Forces Uses for Nuclear Physics Decay Nuclear Stability Einstein’s Famous Equation $200 $300 $400 $500 $400 $300 $200 $100 $500.
Chapter 29:Nuclear Physics
Wilhelm Rontgen 1895 German Scientist Playing with a Crookes tube
Phys 102 – Lecture 27 The strong & weak nuclear forces.
Nuclear Fission and Fusion Unit 8 – Part B. Nuclear Balance Delicate balance between attractive strong nuclear forces and repulsive electric forces. In.
Binding energy sketch the variation of binding energy per nucleon with nucleon number. explain what is meant by nuclear fusion and nuclear fission. explain.
5.3.4 Nuclear Fission and Fusion. (a) select and use Einstein’s mass–energy equation ΔE = Δmc 2.
October 14 DO NOW: Announcements: If you received a check (7.5/10) on the percent error W.S. That is being modified to a check + (10/10) in Skyward. Important.
Nuclear reactions Chapter 17. Standard Describe nuclear reactions and identify the properties of nuclei undergoing them.
Nuclear Energy Nuclear Structure and Radioactivity.
Nuclear Chemistry. ATOMIC REVIEW: Atomic number = # of protons # of neutrons = mass # - atomic # protons & neutrons are in the nucleus.
Nuclear Physics. Nuclear Structure Nucleus – consists of nucleons (neutrons and protons) Nucleus – consists of nucleons (neutrons and protons) Atomic.
Mass Spectrographs and Isotopes. Isotopes Isotopes are atoms of the same kind (same number of protons – same atomic number) which differ in their atomic.
Section 2Nuclear Changes Section 2: Nuclear Fission and Fusion Preview Key Ideas Bellringer Nuclear Forces Nuclear Fission Chain Reaction Nuclear Fusion.
Nuclear, i.e. pertaining to the nucleus. Nucleus Most nuclei contain p + and n 0 When packed closely together, there are strong attractive forces (nuclear.
Unit 13: The nucleus of an atom We know that atoms are composed of electrons, protons and neutrons. Protons and neutrons together (i.e. the nucleus) are.
Honors Physics Chapter 25: Subatomic Physics.  Nucleons  Protons and Neutrons that Make Up the Nucleus  Atomic Number (Z)  # of Protons  Atomic Mass.
II. The Nucleus of the Atom. What makes up the nucleus of an atom? A. Compostion (Nucleons) 1. Protons a. Mass universal mass units b. Indicated.
SACE Stage 2 Physics The Structure of the Nucleus.
Tony Clevenger Office: 104 Office Hours: After Class or By Appointment.
Nuclear Fission and Fusion. Nuclear Reactions Nuclear reactions deal with interactions between the nuclei of atoms Both fission and fusion processes deal.
 Large nuclei (> 92 protons) are unstable and usually results in radioactive decay.  Very rarely a large nucleus will split up spontaneously into two.
By the end of this presentation, you should be able to: Select and use Coulomb’s law to determine the force of repulsion, and Newton’s law of gravitation.
Nuclear Physics An Introduction. What does it mean when something is “Radioactive”? Atomic nuclei that emit particles and energy are said to be radioactive.
Nuclear Stability You should be aware that: A nucleus can be naturally unstable Instability can be induced into a nucleus – for example if we bombard.
Nuclear Physics Lecture 1& 2 © 2015, 2016.
E = mc2 If you can’t explain it simply, you haven’t learned it well enough. Einstein.
Fundamental Forces of the Universe
Fundamental Forces of the Universe
Nuclear Binding, Radioactivity
PHYS 172: Modern Mechanics Summer 2012
Nuclear Energy Nuclear Structure and Radioactivity.
Presentation transcript:

Fall 2010 PHYS 172: Modern Mechanics Lecture 11 – The Energy Principle Chapter 6.15 – 6.17, 7.1 – 7.2 ANNOUNCEMENT The Final Exam in Phys 172H is scheduled for Wednesday, December 15th, from 8:00 am to 10:00 am in Room 114. Note that this is 1.5 hours earlier than our lectures

Mass and energy Example: electron and positron (antielectron) annihilation: neutron electron proton antineutrino Example: neutron decay Mass of products < mass of neutron! Missing mass is converted into kinetic energy Positron tomography All mass is converted into electromagnetic radiation – gamma rays

Mass and energy Mass and energy are the same thing! There is no “mass conservation law”! Energy, not mass is conserved! But only if you do COMPLETE bookkeeping

Mass of a multiparticle system system Mass of a multiparticle system: For example, the mass of a proton is MOSTLY kinetic energy – the three “valence” quarks in the proton have rest masses totaling less than 100 MeV/c 2, while the proton’s mass is 938 MeV/c 2.

i>Clicker question 1 O 2 molecule is oscillating: Mass of the molecule is: A)Larger than total mass of two noninteracting oxygen atoms B)Smaller than total mass of two noninteracting oxygen atoms C)The same as mass of two noninteracting oxygen atoms

i>Clicker question 2 O 2 molecule is oscillating: Mass of the molecule is: A)Larger when atoms are further apart B)Larger when atoms are closer to each other C)Larger when atoms are moving faster D)It does not change during oscillation

Two ways of thinking 1.The energy of a multiparticle system consists of the individual particle energies plus their pair-wise interactions 2.A system itself has energy, like a single particle, and if the system is at rest (not individual objects within the system!) its energy E = Mc 2, where M is mass of the system.

Clicker 1. What happens with the mass of an object when you heat it up? A)It increases B)It decreases C)It does not change Why don’t we notice it? What is the change in mass when we heat up 1 kg of water from 0C to 100C? Later we will learn that energy Q = 4.2  10 5 J is needed to heat it 0 C: kg 100 C: kg

Binding energy: nuclear reactions Proton: m = u Neutron: m = u Deuteron: m = u Adding these, get u Difference is u Binding energy,  mc 2 =2.2MeV (1 eV = 1  J)

The Curve of Nuclear Binding Energy The strong nuclear force attracts nucleons to each other. Nucleons are the generic name for neutrons and protons. The Pauli Exclusion Principle says building block particles (like nucleons or electrons) can’t occupy exactly the same states, so the way nucleons like to combine is with two neutrons and two protons in the ground state (where spin up and spin down distinguish one neutron from the other, ditto for the protons.) So Helium (ppnn) is especially tightly bound, by about 7 MeV per nucleon. This also works well for C-12 and O-16, for example, which are very stable isotopes made from three or four helium nuclei stuck together, speaking loosely. And so on up to Iron, with 56 nucleons. Iron has the greatest binding energy, ~8.7 MeV

The Curve of Nuclear Binding Energy BUT the electrical Coulomb repulsion of the protons from each other tends to work AGAINST binding. Also, this electrical UN- binding energy grows as the SQUARE of the number of protons [each PAIR of protons has its own POSITIVE electrical potential energy.] This requires an excess of neutrons whose strong attraction counteracts the Coulomb repulsion and helps bind the nucleus. Even so, the binding energy per nucleon for elements above Iron in the periodic table is LESS than it is for Iron, which is the most tightly bound nucleus known. The Uranium-235 nucleus has 92 protons and the rest are neutrons (143 in number). It is very weakly bound, and acts like a large liquid drop. Adding one more neutron makes it unstable against “fission” – the drop breaks apart into two droplets, or “fission fragments”, Since the binding energy per nucleon is LARGER for the fragments than for the parent Uranium, the excess is released as Kinetic Energy. This is the source of nuclear power.

Fission and fusion The strong force causes nucleons to attract each other. When nucleons combine into nuclei, energy is released. This is called the binding energy. Iron is the most tightly bound so when elements up to Iron are made by the fusion of light elements energy is released. Similarly if we can break a very heavy atom into lighter elements there is kinetic energy released. E = mc 2 Mass is another form of energy a nucleus is lighter than the sum of the constituent nucleon masses Fusion processes are how the sun produces energy and fission processes are how nuclear reactors produce energy

Nuclear fission slow neutron This process generates more than 1 neutron. These neutrons can initiate further fissions in the Uranium: chain reaction Convert 1 pound into energy – enough to power one household for 100,000 years! 0.454kg x(3E8m/s) 2 = 4.1E16J Power = 4.1E16J/(piE7xE5s) = 1.3E4 Watts = 13kW

Energy versus forces Energy: predict some aspects of motion Limits of possible Less details

Potential energy of a spring x Potential energy of a spring: Take U s = 0 for relaxed spring y

Interatomic potential energy between two atoms Spring-mass model: Problem: energy becomes infinite at large distances and there are no bound states! The Morse potential energy function is a realistic approximation Spring approximation:

Energy of an oscillating spring-mass system x Neglect friction: y x max -x max Maximum speed: Speed at any point:

HOME STUDY: Example, “a rebounding block” k s = 2000 N/m System: block, spring, Earth Assume: no interaction with surroundings  = 1 1. What is the lowest point reached by the block? L0=L0= One equation, one unknown 2. What is the highest point reached by the block? One equation, one unknown See details in the book (7.3), p What facts do we apply to get Eq. 2 ? --- since v i is downward in (1) ??