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Make a sketch of I as a function of X for fixed Z. ( c ) Use the vector formula ( 9.82
) to obtain a result equivalent to that of part ( a ) . Compare the two expressions .
9.7 A linearly polarized plane wave of amplitude E , and wave number k is ...
ot be below which our approximate result ( 13.2 ) must be replaced by a more
exact expression which tends to ( 13.5 ) as b 0. It can be shown ( Problem 13.1 )
that a proper treatment gives the more accurate result , 2z2e4 1 ΔΕ ( b ) ( b ) - (
13.7 ) ...
O angular dependence which is a wellknown result . We note from ( 14.18 ) that
the radiation is polarized in the plane containing ý and n . The total instantaneous
power radiated is obtained by integrating ( 14.21 ) over all solid angle . Thus 2 e
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
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