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3 3 i = 1 j = 1 Evidently the terms in the volume integral ( 6.93 ) transform like
vectors . ... instead of the vectorial form ( 6.93 ) , the tensor can be handled within
the framework of vector operations by introducing a corresponding dyadic .
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 ...
Vector potential , for time - varying fields , 179 in magnetostatics , 139 f . in non -
cartesian coordinates , 141 of localized oscillating source , 269 f . of magnetic
dipole , 146 of oscillating electric dipole , 271 of oscillating electric quadrupole ,
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Introduction to Electrostatics
References and suggested reading
Multipoles Electrostatics of Macroscopic Media
6 other sections not shown