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Nuclear Fission. Historic Dates Fission Mechanism Binding Energy Liquid-Drop Model Classification of Heavy Nuclides Prompt Neutrons Delayed Neutrons. Historic Introduction. 1932: The neutron is discovered by J.Chadwick → experiments with neutrons.
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Nuclear Fission • Historic Dates • Fission Mechanism • Binding Energy • Liquid-Drop Model • Classification of Heavy Nuclides • Prompt Neutrons • Delayed Neutrons T8: Fission
Historic Introduction • 1932: The neutron is discovered byJ.Chadwick → experiments with neutrons. • 1939: Bombardment of U gives medium-heavy atoms (Ba), O.Hahn and F.Strassman; L.Meitner explains; E.Fermi and co-workers did not recognize fission. • 1940: Spontaneous Fission (SF) is discovered by G.N.Flerov and K.A.Petrzhak. • 1947: Ternary fission is discovered by Qian Sabqiang and He Zehui. T8: Fission
Basic Notation • Z is the number of protons, charge number or atomic number • N is the number of neutrons • A = Z + N is the number of nucleons,A is called the mass number • is a specific nucleus, X– chem. sym. • is in an excited state T8: Fission
Nuclides and Isotopes • Isotope ≡ atoms with same Z and A • Nuclide = atoms/nuclei with same Z and A and being in a specific energy state • Isomer = long-lived excited states, T8: Fission
Nuclear Energy Production T8: Fission
Fission Process Ternary: 1/400 0.00650.7% T8: Fission
Compound Nucleus T8: Fission
Binding Energy T8: Fission
Energy Release T8: Fission
Fission Energy T8: Fission
Liquid-Drop Model Nuclear force Surface force Coulomb repulsion Stability maximum Spin factor T8: Fission
Fissionable Ratio T8: Fission
Excitation Energy AX A+1X* T8: Fission
Classification of Heavy Nuclides T8: Fission
Examples of Fission T8: Fission
Fission Product Yield T8: Fission
Kinetic Energy Distribution T8: Fission
Energy Released in Fission T8: Fission
Prompt Neutrons 239Pu 235U 233U E = 1 T8: Fission
Prompt Neutron Energy T8: Fission
E 87Br T½ = 54.5s β– (2%) 87Kr* 86Kr + n β– (98%) 87Kr 87Rb 87Sr t Delayed Neutron Precursors T8: Fission
Delayed Neutron Groups T8: Fission
Delayed Neutron Spectra T8: Fission
Microscopic Cross Section Background material detector Δx Reaction rate R = #/(sm2sec) θ Monoenergetic beam of neutrons I = n/(sm2 sec) x detector cross section σ Microscopic cross section σ is defined by R = σ× I × NB [#/(sm2 sec)] = [sm2] ×[#/(sm2sec)]×[#/sm2] σ/A = Probability per nucleus that a neutron in the beam will interact with it T8: Fission
Fission Cross Section T8: Fission
Resonances T8: Fission
235U vs. 238U T8: Fission
The END T8: Fission