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

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Then, using the homogeneous spectrum obtained and assuming the flat flux, the effective cross-section<br />

of each material is calculated by<br />

where<br />

Σ , = γ Σ − ∑ Σ → Φ / Φ<br />

(7.2-11)<br />

tr g,<br />

M g t,<br />

g,<br />

M<br />

s1,<br />

g ' g,<br />

M 1, g'<br />

1,<br />

g<br />

g '<br />

γ = 1<br />

<strong>for</strong> P1 approximation (7.2-12a)<br />

g<br />

g<br />

g<br />

{ 1 − ( tan α ) α }<br />

−1 α g / 3<br />

−1<br />

γ = α tan<br />

/ <strong>for</strong> B1 approx.<br />

g<br />

g<br />

{ 1 − ( tanh α ) α }<br />

−1 α g / 3<br />

−1<br />

γ = α tanh<br />

/ <strong>for</strong> B1 approx. with<br />

g<br />

g<br />

g<br />

g<br />

2<br />

2<br />

2<br />

with α g = B / Σ , if B 2 t , g >0 (7.2-12b)<br />

2<br />

2<br />

2<br />

with α g = −B / Σ , if B 2 t , g

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