Page 26 - Dynamics and Control of Nuclear Reactors
P. 26

CHAPTER


                  The point reactor kinetics

                  equations                                                 3








                  3.1 Neutronics
                  The neutron population in a nuclear reactor is a function of time, position, direction
                  of motion, and energy. Neutrons appear at some position in the reactor as a result of
                  a fission reaction between uranium or plutonium and a neutron from a previous
                  generation. The neutron emerges from the fission reaction with a large kinetic
                                                                        9
                  energy (an energy of around 3MeV or a speed of around 3 10 cm/s). These
                  neutrons undergo elastic and inelastic scattering events with materials in the
                  reactor core (fuel, structure, cladding, coolant, moderator, etc.) and, as a result,
                  lose energy.
                     Most current-generation reactors include a moderator, a material with a high
                  probability of slowing neurons by scattering collisions while absorbing few
                  neutrons. Typical moderators are water, heavy water, and graphite. Reactors with
                  moderators are called thermal neutron reactors. In these reactors, most of the
                                                                          5
                  neutrons slow to energies less than 0.1eV (a speed of around 4 10 cm/s). Fast
                  reactors have no moderator and rely on fissions with fast neutrons. In a thermal
                  reactor, thetimebetween aneutron’sbirth and eventual absorption by a target
                  nucleus is typically 10 to 30 microseconds, andevenfasterin a reactorwithafast
                  neutron spectrum.
                     The most complete neutronic description of a reactor is the Boltzmann transport
                  equation. This equation gives the neutron population as a function of seven indepen-
                  dent variables (time, three position coordinates, energy and two direction vectors).
                  The neutron diffusion model is one-step simpler. In diffusion theory, the direction
                  dependence is removed, leaving a model with five independent variables. Further
                  simplification occurs with eliminating the spatial dependence (treating the reactor
                  as a “point”) and reducing the energy treatment to a single energy group. These
                  simplifications may seem extreme, but the simplified neutronics model has proved
                  suitable for a wide range of reactor simulations.
                     Appendix C provides a brief discussion of basic reactor physics for those who
                  need familiarization or review.






                                                                                          17
                  Dynamics and Control of Nuclear Reactors. https://doi.org/10.1016/B978-0-12-815261-4.00003-2
                  # 2019 Elsevier Inc. All rights reserved.
   21   22   23   24   25   26   27   28   29   30   31