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Regional Basic Professional Training Course in Korea

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<strong>Regional</strong> <strong>Basic</strong> <strong>Professional</strong> <strong>Tra<strong>in</strong><strong>in</strong>g</strong> <strong>Course</strong> (BPTC) on Nuclear Safety<br />

The easiest approximation of prompt neutron spectra is a Maxwellian approximation<br />

(evaporation spectrum) characterized by a temperature (which depends <strong>in</strong> this case upon<br />

the fission<strong>in</strong>g system and upon <strong>in</strong>cident neutron energy).<br />

with the follow<strong>in</strong>g relationship between average energy and the temperature:<br />

= 1.5 T M<br />

Nevertheless, the Maxwell approximation neglects some physical effects (motion of<br />

fission fragments emitt<strong>in</strong>g neutrons…) A better approximation is the Watt spectrum,<br />

which is <strong>in</strong> fact a centre-of-mass Maxwellian spectrum, transformed to the laboratory<br />

system, assum<strong>in</strong>g an average k<strong>in</strong>etic energy per nucleon Ef. The Maxwellian spectrum is<br />

the limit of the Watt spectrum when Ef tends to 0 (immobile fragment).<br />

with the follow<strong>in</strong>g relationship between average energy and the temperature:<br />

= �f + 1.5TM.<br />

Better (and more complicated) approximations, like the Madland and Nix model, are used<br />

<strong>in</strong> the evaluated files to describe the fission spectrum of the most important fissile<br />

nuclides ( 235<br />

U, 239<br />

Pu).<br />

❙ 32 ❙

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