For a “black disk” absorber, as in Equation 11.34,
R/X
0 = (2e+ i)n~~ = n(~ + A)’ (11.34)
e= o
in which all partial waves
are completely absorbed up to
d= R/X (qe= 0 for complete absorption)
and unaffected for
t‘> R/X ( qe = l), then
uSc = T(R + A)’
(11.49)
and
so that
ur =’a@ + A)’
(11 -50)
ut = 2v(R + A)’ (11.51)
derive black disk scattering
1
Expert's answer
2018-05-21T09:28:54-0400
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