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Page Title: Figure 2 Heatup Stress Profile
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PRESSURIZED THERMAL SHOCK
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Material Science Volume 2 of 2
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Locations  of  Primary  Concern

Thernal Shock DOE-HDBK-1017/2-93 PRESSURIZED THERMAL SHOCK Stresses   arising   from   coolant   system   pressure Figure 2   Heatup Stress Profile exerted   against   the   inside   vessel   wall   (where neutron fluence is greatest) are always tensile in nature. Stresses    arising    from    temperature gradients  across  the  vessel  wall  can  either  be tensile  or  compressive.    The  type  of  stress  is  a function of the wall thickness and reverses from heatup to cooldown.   During system heatup, the vessel outer wall temperature lags the inner wall temperature. The   stresses   produced   by   this temperature gradient and by system pressure will produce the profile shown in Figure 2. During  heatup,  it  can  be  seen  that  while  the pressure  stresses  are  always  tensile,  at  the  1/4 thickness  (1/4  T),  the  temperature  stresses  are compressive.     Thus,  the  stresses  at  the  1/4  T location tend to cancel during system heatup.  At the  3/4  T  location,  however,  the  stresses  from both temperature and pressure are tensile and thus, reinforce each other during system heatup. For this reason the 3/4 T location is limiting during system heatup. During  system  cooldown,  the  stress  profile  of Figure 3   Cooldown Stress Profile Figure 3 is obtained.  During cooldown, the outer wall lags the temperature drop of the inner wall and  is  at  a  higher  temperature.    It  can  be  seen that  during  cooldown,  the  stresses  at  the  3/4  T location  are  tensile  due  to  system  pressure  and compressive   due   to   the   temperature   gradient. Thus during  cooldown, the  stresses at the  3/4 T location  tend  to  cancel.    At  the  1/4  T  location, however,  the  pressure  and  temperature  stresses are both tensile and reinforce each other.   Thus, the   1/4   T   location   is   limiting   during   system cooldown. Plant temperature transients that have the greatest potential   for   causing   thermal   shock   include excessive   plant   heatup   and   cooldown,   plant scrams,   plant   pressure   excursions   outside   of normal   pressure   bands,   and   loss   of   coolant accidents (LOCAs).  In pressurized water reactors (PWRs), the two transients that can cause the most severe thermal shock to the reactor pressure vessel are the LOCA with subsequent injection of  emergency  core  cooling  system  (ECCS)  water  and  a  severe  increase  in  the  primary-to- secondary heat transfer. Rev. 0 Page 7 MS-03

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