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NUREG/CR-5625 (ORNL-6698) - Oak Ridge National Laboratory

NUREG/CR-5625 (ORNL-6698) - Oak Ridge National Laboratory

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Procedure<br />

The technical basis for these characteristics is presented in<br />

Sect. 6.1.<br />

The specific power of cycle i, or e (last cycle), in kW/kgU,<br />

using burnup in MWd/kgU, is defined as<br />

P i<br />

' 1000 B i<br />

0.8 T i<br />

for i < e ;<br />

P e<br />

' 1000 B e<br />

T e<br />

for i ' e .<br />

P ave<br />

'<br />

1000 B tot<br />

.<br />

e & 1<br />

T e<br />

% 0.8 j i ' s<br />

T i<br />

P ave,e & 1<br />

' 1000(B tot & B e )<br />

0.8(T res<br />

& T e<br />

)<br />

.<br />

(2)<br />

The average specific power over the entire operating<br />

history of a fuel assembly, using the same units as in Eq.<br />

(2), is defined as<br />

(3)<br />

The average specific power through the next to last cycle<br />

is used in applying the adjustment factor for short cooling<br />

time (see Sect. 5.2.2). This parameter is defined as<br />

(4)<br />

Note that B tot and P ave , as derived in these definitions, are<br />

used in determining the heat generation rate from the<br />

guide. Also, for cooling times #7 years, P e is used in an<br />

adjustment formula. The method applied here<br />

accommodates storage of a fuel assembly outside the<br />

reactor during one or two cycles and returning it to the<br />

reactor. Then, B i = 0 may be set for all intermediate<br />

storage cycles. If the cooling time is short (i.e.,

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