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James A. Van Allen lab journal, September 1959-January 1961
Page 191
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beam (by re-radiation) may be calculated : R=radiation resistance (?) { Power re-radiated time average = ((((E {[emf?]}) sub 0) exponent 2)/(2R)) = (((4)(pi exponent 2)((E sub 0) exponent 2)(A exponent 2))/(2R(lambda exponent 2))) R is a function of A of course - ] The effective "cross-section" of the loop is = ((Power Re-radiated)/(|[Poynting?] Vector|)) By Moullin, page 26 R= (((320)(pi exponent 4)(A exponent 2))/(lambda exponent 4)) ohms. The result for power re-radiated (or scattered
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beam (by re-radiation) may be calculated : R=radiation resistance (?) { Power re-radiated time average = ((((E {[emf?]}) sub 0) exponent 2)/(2R)) = (((4)(pi exponent 2)((E sub 0) exponent 2)(A exponent 2))/(2R(lambda exponent 2))) R is a function of A of course - ] The effective "cross-section" of the loop is = ((Power Re-radiated)/(|[Poynting?] Vector|)) By Moullin, page 26 R= (((320)(pi exponent 4)(A exponent 2))/(lambda exponent 4)) ohms. The result for power re-radiated (or scattered
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