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Page Title: Core Burnup
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Nuclear Physics and Reactor Theory Volume 2 of 2
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REACTOR OPERATION DOE-HDBK-1019/2-93 Reactor Theory (Reactor Operations) Flow At low reactor power levels, changing the flow rate of the coolant through the reactor does not result in a measurable reactivity change because fuel and moderator temperatures and the fraction of steam voids occurring in the core are not changed appreciably. When the flow  rate is  varied, however, the change in  temperature that occurs  across  the core (outlet versus inlet temperature) will vary inversely with the flow rate.   At higher power levels, on  liquid  cooled  systems,  increasing  flow  will  lower  fuel  and  coolant  temperatures  slightly, resulting in a small positive reactivity insertion. A positive reactivity addition also occurs when flow is increased in a two-phase (steam-water) cooled system. Increasing the flow rate decreases the  fraction  of  steam  voids  in  the  coolant  and  results  in  a  positive  reactivity  addition.    This property  of  the  moderator  in  a  two-phase  system  is  used  extensively  in  commercial  BWRs. Normal power variations required to follow load changes on BWRs are achieved by varying the coolant/moderator flow rate. Core  Burnup As a reactor is operated, atoms of fuel are constantly consumed, resulting in the slow depletion of the fuel frequently referred to as core burnup.   There are several major effects  of this fuel depletion.   The first, and most obvious, effect of the fuel burnup is that the control rods must be withdrawn or chemical shim concentration reduced to compensate for the negative reactivity effect of this burnup. Some reactor designs  incorporate the use of  supplemental burnable poisons  in addition to  the control rods to compensate for the reactivity associated with excess fuel in a new core.   These fixed  burnable  poisons  burn  out  at  a  rate  that  approximates  the  burnout  of  the  fuel  and  they reduce the amount of control rod movement necessary to compensate for fuel depletion early in core life. As control rods are withdrawn to compensate for fuel depletion, the effective size of the reactor is increased.  By increasing the effective size of the reactor, the probability that a neutron slows down and is absorbed while it is still in the reactor is also increased.  Therefore, neutron leakage decreases  as  the effective reactor size is increased.   The magnitude of the moderator negative temperature coefficient is determined in part by the change in neutron leakage that occurs as the result of a change in moderator temperature.   Since the fraction of neutrons leaking out is less with  the  larger  core,  a  given  temperature  change  will  have  less  of  an  effect  on  the  leakage. Therefore, the magnitude of the moderator negative temperature coefficient decreases with fuel burnup. NP-04 Rev. 0 Page 30

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