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Resonance escape probability average

In these and the above equations, the a are cross sections per imit volume, the a in (8) is scattering cross section, the average loss in r per collision. The are used because the material may contain different types of atoms. The (Ta is the thermal absorption cross section r(r) the resonance absorption cross section per unit volume. The = qef is the multiplication constant divided by the resonance escape probability. The product of thermal utilization / and (Ta is the effective cross section of uranium per unit volume, i.e., its cross section per unit volume multiplied by the thermal neutron density in it and divided by the average thermal neutron density. One can write, therefore, (Tu for f(Ta- If one multiplies this with rj the result is the same as crfU where fission cross section for thermal neutrons per unit volume, p the number of fast neutrons per fission. As a result, the third term in (7) can be written also as e is the multiplication by fast effect)... [Pg.543]

This result may be written in a more compact manner by introducing an average resonance escape probability for neutrons released according to the fission spectrum thus,... [Pg.153]


See other pages where Resonance escape probability average is mentioned: [Pg.125]    [Pg.106]    [Pg.106]    [Pg.109]    [Pg.110]    [Pg.278]    [Pg.316]    [Pg.633]    [Pg.241]    [Pg.70]    [Pg.906]    [Pg.388]    [Pg.11]   
See also in sourсe #XX -- [ Pg.153 ]




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