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JAEA-Data/Code 2007-004 - Welcome to Research Group for ...

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2.10 Reaction Rate Calculation<br />

The input of this section is optionally required if IC18=1 (Sect.2.2) is specified <strong>for</strong> the reaction<br />

rate calculation.<br />

A common edit can be executed after any component routine <strong>for</strong> flux distribution (PIJ, ANISN,<br />

TWOTRAN, TUD or CITATION). The edit routine REACT permits the calculation of reaction<br />

(capture, fission) rate distribution of the detec<strong>to</strong>r with or without the filter.<br />

(a) The reaction rate (cm -3 sec -1 ) of the detec<strong>to</strong>r without filter is calculated as follows:<br />

r<br />

R(<br />

) =<br />

IGMAX<br />

∑<br />

g=<br />

1<br />

r<br />

Σ x, gΦg(<br />

)<br />

(2.10-1)<br />

where IGMAX is number of energy group, and x means reaction type (e.g. capture, fission, etc.).<br />

(b) The reaction rate (cm -3 s -1 ) of the detec<strong>to</strong>r with filter:<br />

r<br />

R(<br />

) =<br />

IGMAX<br />

∑<br />

g=<br />

1<br />

r<br />

f g Σ Φg(<br />

x, g )<br />

, where f g is filter transmission fac<strong>to</strong>r (2.10-2)<br />

By adjusting f g , the integration range can be modified. The reaction types edited by (a) and (b)<br />

are Fission, Capture and Absorption (A=F+C).<br />

(c) Spectrum index<br />

As shown in the following equations (2.10-3) through (2.10-8), the fission reaction rate (F),<br />

capture rate (C) of nuclide μ in epi-thermal range (epi), thermal energy range (th) and whole energy<br />

range (all) are calculated as:<br />

F = ∫ ∞<br />

N<br />

μ σ μ ( E)<br />

ϕ(<br />

E)<br />

dE , (2.10-3)<br />

epi<br />

E Cd<br />

f<br />

μ , (2.10-4)<br />

F<br />

th<br />

= ∫<br />

0<br />

E Cd<br />

μ<br />

N σ μ ( E)<br />

ϕ(<br />

E)<br />

dE<br />

f<br />

μ , (2.10-5)<br />

μ<br />

all<br />

μ<br />

th<br />

F = F + F<br />

μ<br />

epi<br />

C = ∫ ∞<br />

N<br />

μ σ μ ( E)<br />

ϕ(<br />

E)<br />

dE , (2.10-6)<br />

epi<br />

E Cd<br />

c<br />

μ , (2.10-7)<br />

C<br />

th<br />

= ∫<br />

0<br />

E Cd<br />

μ<br />

N σ μ ( E)<br />

ϕ(<br />

E)<br />

dE<br />

c<br />

μ 129

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