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Fission Product Yield Data for the Transmutation of Minor Actinide ...

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For <strong>the</strong> dip at A = 130:<br />

n ( A) = I [ e D ] / pC<br />

H D<br />

142<br />

-( A-130) C 2 /<br />

(4.2.22f)<br />

I D = –5.0 (4.2.22g)<br />

C D = 2.0(3.0 2 + 1/12) = 18.17 (4.2.22h)<br />

For <strong>the</strong> light dip complementary to A = 130:<br />

n ( A) = I [ e C D]<br />

/ pC<br />

L D<br />

(4.2.22i)<br />

S C = A F – 130.0 – (V F – D H + S H ) (4.2.22j)<br />

DH = ID/ pCD<br />

2 -( A-S ) / C<br />

S = I [ e D ] / pC<br />

H D<br />

2 /<br />

-( 130. 0-SYM)<br />

C<br />

(4.2.22k)<br />

(4.2.22l)<br />

SYM = (A F – n s )/2.0 (4.2.22m)<br />

4.2.4.5. Model <strong>for</strong> R(A)<br />

Generalized R(A) functions consist <strong>of</strong> a<br />

number <strong>of</strong> straight line segments chosen to give<br />

sawtooth n A (A) functions with some inflections.<br />

Two R(A) functions are shown in Figs 4.2.39 and<br />

4.2.40, and equations <strong>for</strong> <strong>the</strong> segments in <strong>the</strong> various<br />

regions designated in Figs (4.2.39) and (4.2.40) are<br />

given below. Note that Eqs (4.2.23c) and (4.2.23f)<br />

are excitation energy dependent continuous<br />

functions that approximate <strong>the</strong> <strong>for</strong>mer discrete<br />

values [4.2.4, 4.2.29].<br />

A < D: R(A) = 0.20 (4.2.23a)<br />

A = D to F: R(A) = 0.2 + (A – D)(R(F) – 0.2)/(F – D)<br />

(4.2.23b)<br />

A = F to G: R(A) = 0.9 – 0.0075(PE) (4.2.23c)<br />

A = G to H: R(A) = 0.5 + (H – A)(R(G) – 0.5)/(H – G)<br />

(4.2.23d)<br />

A = H to J: R(A) = 0.5 – (A – H)(0.5 – R(J))/(J – H)<br />

(4.2.23e)<br />

A = J to K: R(A) = 0.1 + 0.0075(PE) (4.2.23f)<br />

D<br />

D<br />

D<br />

FIG. 4.2.39. Fraction R(A) <strong>of</strong> n T (A) to A <strong>for</strong> U235T.<br />

FIG. 4.2.40. Fraction R(A) <strong>of</strong> n T(A) to A <strong>for</strong> 238 U + 85 MeV p.<br />

A = K to M:<br />

R(A) = R(K) + (A – K)(0.8 – R(K))/(M – K) (4.2.23g)<br />

A > M: R(A) = 0.80 (4.2.23h)<br />

The n A (A) functions derived from <strong>the</strong> above<br />

equations <strong>for</strong> two fission reactions are compared<br />

with <strong>the</strong> experimental data in Figs 4.2.41 and 4.2.42<br />

(U235T: Refs [4.2.39-4.2.42]; CF252S: Refs [4.2.43–<br />

4.2.47]). As can be seen, <strong>the</strong> model n A (A) functions<br />

represent <strong>the</strong> data moderately well, and to <strong>the</strong> same<br />

extent as <strong>the</strong> different data sets <strong>for</strong> each fission<br />

reaction agree with each o<strong>the</strong>r. The inflection in <strong>the</strong><br />

n A(A) model function near A = 105 is also exhibited<br />

by <strong>the</strong> data, and is related to <strong>the</strong> light dip in <strong>the</strong><br />

n T (A) function. The significant dip in n T (A) is<br />

rein<strong>for</strong>ced by <strong>the</strong> minimum <strong>of</strong> R(A) at J to K to give<br />

<strong>the</strong> n A (A) minimum just below A = 130. The above<br />

equations are used in <strong>the</strong> CYF yield calculation<br />

program.

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