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Page Title: Maximum Local Linear Power Density
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Thermal Limits
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Thermodynamics Heat Transfer and Fluid Flow Volume 2 of 3
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Figure 17    Radial Temperature Profile Across a Fuel Rod and Coolant Channel

HEAT GENERATION Heat Transfer Maximum Local Linear Power Density The  maximum  local  linear  power  density  when  compared  to  the  average  linear  power  density results in the definition of the nuclear heat flux hot channel factor.   The nuclear heat flux hot channel factor can be looked at as having axial and radial components that are dependent upon the power densities and, thus, the flux in the radial and axial planes of the core.   Once the hot channel factor is known, the maximum local linear power density anywhere in the core can be determined, as demonstrated in the following example. Example: If  the  nuclear  heat  flux  hot  channel  factor  is  1.83,  calculate  the  maximum  local  linear power  density  in  the  core  for  the  previous  example  (the  average  linear  power  density problem). Solution: Maximum linear power density =   HFHCF (Av linear power density) =   1.83 (5.56) kW/ft =   10.18 kW/ft Normally,   nuclear   facility   operators Figure 16    Axial Temperature Profile are   provided   with   the   above   core power and heat generation distributions,   rather   than   having   to calculate  them.    In  addition,  various monitoring systems are always employed to provide the operator with a means of monitoring core performance and the proximity of the existing  operating  conditions  to  core operational limitations. Temperature Profiles Additional  areas  of  interest  are  the temperature  profiles  found  within  the core.    A    typical    axial    temperature profile  along  a  coolant  channel  for  a pressurized   water   reactor   (PWR)   is shown  in  Figure  16.    As  would  be expected,    the    temperature    of    the coolant will increase throughout the entire length of the channel. HT-02 Page 48 Rev. 0

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