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Page Title: Flow Rate and Temperature Difference
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Conditions Required for Natural Circulation
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Thermodynamics Heat Transfer and Fluid Flow Volume 3 of 3
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Natural Circulation Flow Summary

Fluid Flow NATURAL CIRCULATION The two areas must be in contact so that flow between the areas is possible.   If the flow path is obstructed or blocked, then natural circulation cannot occur. Example of Natural Circulation Cooling Natural  circulation  is  frequently  the  primary  means  of  cooling  for  pool-type  reactors  and  for irradiated  fuel  assemblies  stored  in  pools  of  water  after  removal  from  the  reactor.    The  heat source is the fuel assembly.   The heat sink is the bulk of the water in the pool. Water at the bottom of a fuel assembly absorbs energy generated by the assembly.   The water increases in temperature and decreases in density.   Gravity pulls cooler (more dense) water into the bottom of the assembly displacing the warmer water.   The warmer (lighter) water is forced to give up its position to the cooler (heavier) water.   The warmer (lighter) water rises higher in the assembly.  As water travels up the length of the assembly, it absorbs more energy.  The water becomes lighter and lighter being continuously forced upward by more dense water moving in below it. In turn, the cooler water absorbs energy from the assembly and is also forced to rise as  natural  circulation  flow  continues.   Water  exiting  the  top  of  the  fuel  assembly  gives  up  its energy as it mixes with the bulk of the water in the pool.   The bulk of the water in the pool is commonly cooled by circulation through heat exchangers in a separate process. Flow Rate and Temperature Difference The thermal driving head that causes natural circulation is due to the density change caused by a temperature difference.  In general, the greater the temperature difference between the hot and cold areas of fluid, the greater the thermal driving head and the resulting flow rate.   However, it is good practice to keep the hot fluid subcooled to prevent a change of phase from occurring. It  is  possible  to  have  natural  circulation  take  place  in  two-phase  flow,  but  it  is  usually  more difficult to maintain flow. Various  parameters  can  be  used  to  indicate  or  verify  natural  circulation  is  occurring.   This  is dependent on plant type.   For instance for a pressurized water reactor (PWR) selected Reactor Coolant System (RCS) parameters that would be used are as follows. 1. RCS  DT  (THot  -  TCold)  should  be  25-80%  of  the  full  power  value  and  either  steady  or slowly decreasing.   This indicates that the decay heat is being removed from the system at an adequate rate to maintain or reduce core temperatures. 2. RCS Hot and Cold leg temperatures should be steady or slowly decreasing.   Again, this indicates that heat is being removed and the decay heat load is decreasing as expected. 3. Steam  generator  steam  pressure  (secondary  side  pressure)  should  be  following  RCS temperature.    This  verifies  that  the  steam  generator  is  removing  heat  from  the  RCS coolant. If natural circulation for a PWR is in progress or is imminent, several actions can be performed to ensure or enhance core cooling capabilities.  First, pressurizer level can be maintained greater than 50%.   Secondly, maintain the RCS subcooled by 15oF or greater. Rev. 0 Page 39 HT-03

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