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