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DECAY HEAT
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Thermodynamics Heat Transfer and Fluid Flow Volume 2 of 3
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Calculation of Decay Heat

Heat Transfer DECAY HEAT The design of the reactor must allow for the removal of this decay heat from the core by some means.   If adequate heat removal is not available, decay heat will increase the temperatures in the core to the point that fuel melting and core damage will occur.   Fuel that has been removed from  the  reactor  will  also  require  some  method  of  removing  decay  heat  if  the  fuel  has  been exposed to a significant neutron flux.  Each reactor facility will have its own method of removing decay heat from both the reactor core and also any irradiated fuel removed from the core. Calculation of Decay Heat The amount of decay heat being generated in a fuel assembly at any time after shutdown can be calculated in two ways.   The first way is to calculate the amount of fission products present at the  time  of  shutdown.   This  is  a  fairly  detailed  process  and  is  dependent  upon  power  history. For a given type of fuel, the concentrations, decay energies, and half lives of fission products are known.   By starting from a known value, based on power history at shutdown, the decay heat generation rate can be calculated for any time after shutdown. An   exact   solution   must   take   into   account   the   fact   that   there   are   hundreds   of   different radionuclides  present  in  the  core,  each  with  its  own  concentration  and  decay  half-life.    It  is possible  to  make  a  rough  approximation  by  using  a  single  half-life  that  represents  the  overall decay  of  the  core  over  a  certain  period  of  time.   An  equation  that  uses  this  approximation  is Equation 2-16. (2-16) Q Qo æ ç è ö ÷ ø 1 2 time half   life where: = decay heat generation rate at some time after shutdown Q = initial decay heat immediately after shutdown Qo time = amount of time since shutdown half-life = overall decay half-life of the core Rev. 0 Page 53 HT-02

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