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CHAPTER

                                                                            7
                  Reactivity feedbacks











                  7.1 Basics
                  Changes in power reactor temperature or pressure cause reactivity changes. The
                  causes for these reactivity changes are the temperature dependence of nuclear prop-
                  erties, changes in the quantity of material present in the reactor core because of den-
                  sity changes or changes in the dimensions or shape of core components. Evaluating
                  the feedback reactivity involves the use of feedback coefficients (change in reactivity
                  per unit change in a process variable). Feedback reactivity effects are very important
                  in achieving suitable reactor performance.
                     This chapter addresses a qualitative description of relevant effects. Quantitative
                  evaluation of feedback coefficients requires use of detailed neutronic models. These
                  methods are described in books on reactor physics [1] and are beyond the scope and
                  purpose of this book. Here, it will be assumed that analysts will be provided with
                  reactivity coefficients needed to perform a dynamic simulation.
                     The following sections address reactivity feedbacks in general for thermal reac-
                  tors, specifically for thermal reactors that are so-called Generation II and Generation
                  III reactors.




                  7.2 Fuel temperature feedback in thermal reactors
                  Fuel temperature affects reactivity through changes in Doppler broadening of
                  absorption resonances. Some fission neutrons are lost during slowing down as a
                  result of absorption in heavy isotopes (principally U-238 and Pu-240 in thermal reac-
                  tors with low-enrichment uranium fuel). Resonances in their absorption cross sec-
                  tions cause a decrease in the number of neutrons reaching thermal energy (the
                  resonance escape probability decreases).
                     Changes in temperature change the relative motion between the resonance
                  absorber and a neutron. This causes a reduction in the peak of the absorption cross
                  section and a broadening over a wider range of energies. See Fig. 7.1.
                     Since the cross section is still very large in the broadened region, the heavy iso-
                  tope absorbs more neutrons than would be absorbed in an unbroadened resonance.
                  This increased resonance absorption causes reactivity to decrease. The effect
                  occurs in U-238 and is even stronger in Pu-240 as it builds up by absorptions in
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                  Dynamics and Control of Nuclear Reactors. https://doi.org/10.1016/B978-0-12-815261-4.00007-X
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