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Slowing-down Process in the Infinite Medium

This problem was previously encountered in the case of the infinite-medium slowing-down process for a multiplying material. In that instance we identified the source term for the thermal neutrons as the slowing-down density at thermal energy g(i th) [cf. Eq. (4.252)]. In the present case we require a somewhat more generalized function which takes into account the spatial distribution of the slowing-down density. Thus a suitable description for the source term in the diffusion equation for thermal neutrons would be... [Pg.219]

S A point source in an infinite medium is emitting neutrons of zero lethargy isotropically at a constant rate in time. Assume that the slowing-down process may be described by means of the Fermi age model once the first collision has occurred. Thus at points of first collision, the neutrons enter a continuous slowing-down process. [Pg.327]


See other pages where Slowing-down Process in the Infinite Medium is mentioned: [Pg.69]    [Pg.83]    [Pg.85]    [Pg.87]    [Pg.89]    [Pg.91]    [Pg.95]    [Pg.107]    [Pg.109]    [Pg.111]    [Pg.113]    [Pg.115]    [Pg.119]    [Pg.121]    [Pg.123]    [Pg.127]    [Pg.129]    [Pg.131]    [Pg.137]    [Pg.139]    [Pg.149]    [Pg.153]    [Pg.159]    [Pg.69]    [Pg.83]    [Pg.85]    [Pg.87]    [Pg.89]    [Pg.91]    [Pg.95]    [Pg.107]    [Pg.109]    [Pg.111]    [Pg.113]    [Pg.115]    [Pg.119]    [Pg.121]    [Pg.123]    [Pg.127]    [Pg.129]    [Pg.131]    [Pg.137]    [Pg.139]    [Pg.149]    [Pg.153]    [Pg.159]    [Pg.270]    [Pg.88]    [Pg.98]    [Pg.135]    [Pg.26]    [Pg.268]    [Pg.275]    [Pg.284]    [Pg.412]   


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Downs process

Infinite medium

Slow process

Slowing down

The down

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