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Page Title: Fuel Changes During Reactor Operation
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Figure 17    Radial Temperature Profile Across a Fuel Rod and Coolant Channel
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Thermodynamics Heat Transfer and Fluid Flow Volume 2 of 3
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Heat Generation Summary

HEAT GENERATION Heat Transfer Volumetric Thermal Source Strength The total heat output of a reactor core is called the  heat generation rate.   The heat generation rate divided by the volume of fuel will give the average volumetric thermal source strength.  The volumetric thermal source strength may be used to calculate the heat output of any section of fuel rod, provided the volume of the section is known. Volumetric  Thermal  Source  Strength Qcore Vfuel Fuel Changes During Reactor Operation During the operation of a nuclear reactor, physical changes occur to the fuel that affect its ability to transfer heat to the coolant.  The exact changes that occur are dependant on the type and form of fuel.   Some reactors use fuel assemblies that consist of zircalloy tubes containing cylindrical ceramic pellets of uranium dioxide.   During manufacture, a small space or gap is left between the fuel pellets and the zircalloy tube (clad).   This gap is filled with pressurized helium.   As the reactor  is  operated  at  power,  several  physical  changes  occur  in  the  fuel  that  affect  the  gap between the pellets and clad.  One change occurs due to high pressure in the coolant outside the clad  and  the  relatively  high  temperature  of  the  clad  during  reactor  operation.     The  high temperature and high pressure causes the clad to be pushed in on the pellets by a process referred to as creep.  Another physical change is caused by the fission process.  Each fission event creates two fission product atoms from a fuel atom.   Even though each fission product atom is roughly half the mass of the fuel atom, the fission products take up more volume than the original fuel atom.  Fission products that are gases can collect together and form small gas bubbles within the fuel pellet.   These factors cause the fuel pellets to swell, expanding them out against the clad. So the two processes of pellet swell and clad creep both work to reduce the gap between the fuel and clad. This change in the gap between the pellet and clad has significant impact on heat transfer from the  fuel  and  operating  fuel  temperatures.    Initially  a  significant  temperature  difference  exists across the gap to cause heat transfer to take place by convection through the helium gas.  As the size  of  the  gap  is  reduced,  a  smaller  temperature  difference  can  maintain  the  same  heat  flux. When the fuel pellets and clad come in contact, heat transfer by conduction replaces convection and the temperature difference between the fuel surface and clad decreases even more.   Due to the  processes  of  pellet  swell  and  clad  creep,  the  fuel  temperatures  of  some  reactors  decrease slightly over time while the heat flux from the fuel and therefore the power of the reactor remain constant. Not  all  changes  that  occur  to  the  fuel  during  reactor  operation  work  to  enhance  heat  transfer. If  the  chemistry  of  the  coolant  is  not  carefully  controlled  within  appropriate  limits,  chemical reactions  can  take  place  on  the  surface  of  the  clad,  resulting  in  the  formation  of  a  layer  of corrosion products or crud between the metal of the clad and the coolant.   Typically, this layer will  have  a  lower  thermal  conductivity  than  that  of  the  clad  material,  so  it  will  act  as  an insulating blanket, reducing heat transfer. HT-02 Page 50 Rev. 0

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