Announcements •Answer key for quiz 1 has been posted at websitesee folder called “quizzes 2007”. •Quiz grades, attendance credit will be available at a confidential grade check on the web page later this week. •First mid-term exam from 2006 has been posted at the web site – see folder called “Old Exams”. •Grades for quiz 1 based on the number of correct answers are as follows 5 – A; 4 – B; 3 – C; 2 – D; 1 or 0 - F Supplementary Reading, Nuclear Chemistry • Zumdahl Text, Sections 21.5 – 21.6, pages 993 – 1002 • National Ignition Facility Project http://www.llnl.gov/nif/project/ • International Thermonuclear Experimental Reactor (ITER) http://www.iter.org/a/index_nav_1.htm http://www.iter.org/a/index_nav_2.htm 235U Chain Reaction, Fission Reactor Chicago Pile 1, December 2, 1942, First Sucessful Nuclear Reactor Enrico Fermi, Nobel Prize, 1938 Chain Reaction • http://www.physics.umd.edu/lecdem/servic es/demos/demosp4/p4-62a.mpg • Neutrons are emitted when 235U undergoes fission • These neutrons are then available to trigger fission in other nuclei • This process is called a chain reaction – If uncontrolled, a violent explosion can occur – The principle behind the nuclear bomb, where 1 g of 235U can release energy equal to about “??” tons of TNT Many Radioactive Fragments form in Fission Many radioactive fragments last for many centuries after they are formed Basic Reactor Design • Fuel elements consist of enriched 235U (natural uranium contains 0.7% 235U and 99.3% 238U) • 238U almost never undergoes fission • The moderator material helps to slow down the neutrons • The control rods absorb neutrons To start the reactor the control rods are pulled out of the core To stop the reactor the control rods are pushed into the core Fuel rods Electricity from Nuclear Fission In a fission reactor, enriched Uranium, which is Uranium-238 with a high concentration of Uranium-235, undergoes a process known as Induced Nuclear Fission. Nuclear Fission occurs when an atom of a fissionable material is struck by a neutron and splits into two lighter atoms, releasing a massive amount of heat and gamma radiation. The heat is used to boil water, producing steam used to turn a generator. Nuclear Fission Reactor Nuclear Fusion –A Star Fusion in the Sun • All stars generate energy through fusion • The Sun, along with about 90% of other stars, fuses hydrogen – Some “older” stars fuse heavier elements • Two conditions must be met before fusion can occur in a star – The temperature must be high enough – The density of the nuclei must be high enough to ensure a high rate of collisions The Sun • Source of solar energy • A large nuclear fusion reactor • 1.39x109 m in diameter • ~1.5x1011 m away from us Structure of the Sun Corona: Very Hot Chromosphere: UV Radiation Photosphere: “skin” Convection Zone: Rising and Falling Gas Radiation Zone: X-rays Core: Nuclear Fusion Proton-Proton Chain Considerations for a Fusion Reactor • The proton-proton chain is not feasible for a fusion reactor – The high temperature and density required are not suitable for a fusion reactor – It takes a long, long time for the proton-proton chain reaction to occur – centuries • The most promising reactions involve deuterium and tritium: D-T FUSION D-T Fusion The Process • • Nuclei of two isotopes of hydrogen, deuterium (D) and tritium (T) react to produce a helium (He) nucleus and a neutron (n). In each reaction, 17.6 MeV of energy (2.8 pJ) is liberated: D + T 4He (3.5 MeV) + n (14.1 MeV) Fusion Reactors • Energy releasing fusion reactions are called thermonuclear fusion reactions • A great deal of effort is being directed at developing a sustained and controllable thermonuclear reaction • A thermonuclear reactor that can deliver a net power output over a reasonable time interval is not yet a reality Considerations for a Fusion Reactor • Tritium is radioactive and must be produced artificially • One of the main problems in obtaining energy from nuclear fusion is the fact that the Coulomb repulsion between two charged nuclei must be overcome before they can fuse • This is a competition between long range Coulomb forces and much stronger but very short range strong forces that bind protons and neutrons together binding the nucleus the nucleus of helium contains two protons which are both positively charged. they should repel each other but they are strongly bonded to each other- why? the strong force • an attractive force • has an effect over a very short range (10-15 m, about the size of the nucleus) • leptons don’t feel this force, but particles in the quark family do. strong nuclear force Residual Strong Force • The strong force between the quarks in one proton and the quarks in another proton is strong enough to overwhelm the repulsive electromagnetic force Requirements for Successful Thermonuclear Reactor • High temperature ~ 108 K – Needed to give nuclei enough energy to overcome Coulomb forces – At these temperatures, the atoms are ionized, forming a plasma • Plasma ion density, n – The number of ions present • Plasma confinement time, τ – The time the interacting ions are maintained at a temperature equal to or greater than that required for the reaction to proceed successfully Phases of Fully ionized >106 K Matter Plasma Forms >104 K >103 K Molecules dissociate to atoms Gas Phase >102 K Liquid Phase Solid Phase Controlled Fusion on Earth – Can it be Done? Breeding Tritium in a Fusion Reactor 2 3 4 1 H + H → He + n 1 1 2 0 fast 1 7 3 4 1 n + Li → H + He + n 0 fast 3 1 2 0 slow 1 6 3 4 0 nslow + 3 Li →1 H + 2 He Confinement of Fusion 1. Gravity – A Star 2. Magnetic Tokamak 3. Inertial – Laser Principles of Inertial Confinement Inertial Confinement Fusion Reactor National Ignition Facility (NIF) Hohlraum Target with D-T Pellet Human Scale T ~ 100 million K has been achievedbut only for ~ 10-9 s Operation Principles of a Tokamak T ~ 40 million K has been achieved International Thermonuclear Experimental Reactor (ITER) Human Scale The Future of Controlled Nuclear Fusion The Problem with Energy Conservation Ei Heat, q ∆Efuel ∆Eq ∆Ew Work, w ∆Ef -∆Efuel = ∑∆Eq + ∑∆Ew Piggy Bank Glass is Conserved!
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