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Nuclear Physics and Reactor Theory Volume 1 of 2
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ENERGY RELEASE FROM FISSION

Atomic and Nuclear Physics DOE-HDBK-1019/1-93 NUCLEAR FISSION Nuclear  Fission  Summary The fission process can be explained using the liquid drop model of a nucleus. In the ground state the nucleus is nearly spherical in shape.  After the absorption of  a  neutron,  the nucleus  will  be  in  an  excited  state  and start  to  oscillate  and become distorted.   If the oscillations cause the nucleus to become shaped like a dumbbell,   the   repulsive   electrostatic   forces   will   overcome   the   short-range attractive nuclear forces, and the nucleus will split in two. Excitation energy is the amount of energy a nucleus has above its ground state. Critical energy is the minimum excitation energy that a nucleus must have before it can fission. Fissile material is material for which fission is possible with neutrons that have zero kinetic energy.  Fissionable material is material for which fission caused by neutron absorption is possible provided the kinetic energy added with the binding energy is  greater than the critical energy.   Fertile material is  material that can undergo transmutation to become fissile material. Transmutation is the process of neutron absorption and subsequent decay, which changes one nuclide to another nuclide.  Conversion is the process of transmuting fertile  material  into  fissile  material  in  a  reactor,  where  the  amount  of  fissile material produced is less than the amount of fissile material consumed.  Breeding is the same as conversion, except the amount of fissile material produced is more than the amount of fissile material consumed. The  curve  of  binding  energy  per  nucleon  increases  quickly  through  the  light nuclides  and  reaches  a  maximum  at  a  mass  number  of  about  56.    The  curve decreases slowly for mass numbers greater than 60. The  heaviest  nuclei  are  easily  fissionable  because  they  require  only  a  small distortion from the spherical shape to allow the coulomb forces to overcoming the attractive nuclear force, forcing the two halves of the nucleus apart. Uranium-235 fissions with thermal neutrons because the binding energy released by the absorption of a neutron is greater than the critical energy for fission.  The binding  energy  released  by  uranium-238  absorbing  a  neutron  is  less  than  the critical energy, so additional kinetic energy must be possessed by the neutron for fission to be possible. Rev. 0 Page 55 NP-01

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