Page 258 - Dynamics and Control of Nuclear Reactors
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APPENDIX C Basic reactor physics     259




                     The most probable fission fragments are Cs-140 (Cesium) and Rb-93 (Rubid-
                  ium). For example, the reactions involving these fission fragments are given as
                  follows:
                             235  1  236   140  93    1
                             92 U + n ! 92 U ∗ ! 55 Cs + Rb +3 n + Energy   200 MeVð  Þ  (C.7)
                                  0
                                                      0
                                                37
                  The high-speed fission fragments lose energy by interaction with the molecules of
                  the surrounding medium (fuel, structure, moderator, etc.), thus converting kinetic
                  energy (KE) to thermal energy. There is also heating due to gamma radiation and
                  slowing down of neutrons to lower energy levels. An average of υ¼2.43 neutrons
                  are produced per fission induced by thermal neutrons in U-235.
                     Avogadro’s Number (AN): is the number of molecules per gram mole or atoms
                  per gram atom of a substance. One gram-atom is the quantity of substance in grams,
                  numerically equal to its atomic mass. Avogadro’s Number is numerically equal to
                               23
                  AN¼6.023 10    atoms per gram-atom.

                   Example C.2
                    The number density (N) of U-235 atoms in natural uranium is the number of atoms of U-235
                         3
                    per cm . The number density is given by
                                              N ¼ ANÞ ρe=m
                                                 ð
                    where
                                         3
                       ρ¼material density, gm/cm
                       e¼enrichment [U-235/(U-235+U-238)]
                       m¼gram U per gram atom U.

                     The number density of U-235 in 1% enriched uranium (with a material density of
                          3
                  19.0 g/cm is [3].

                                               23
                        19:0 gramU=cm  3   6:023 10 ð atomsU=gram atomUÞ  atomsU 235
                   N 235 ¼                                         0:01
                                   238 gramU=gram atomUÞ                   atomU
                                      ð
                                            3
                               20
                       ¼ 4:80 10 atoms U-235=cm :
                  Some energy equivalents are as follows:
                     1 eV is the amount of kinetic energy imparted to an electron when accelerated
                  through a potential difference of 1 V.
                     1eV¼1.602 10   19  J
                     1 cal¼4.184 J.
                  The absorption of a neutron by the U-235 nucleus has the form
                                             92 U + n ! 92 U ∗                   (C.8)
                                             235  1  236
                                                  0
                  This results in extra internal energy of the product, because the sum of masses of the
                  two interacting particles is greater than that of a normal U-236 nucleus (at ground
                  state). This excess energy is sufficient to cause nuclear fission (electrostatic repul-
                  sion dominates nuclear attraction).
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