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Similarly it is plausible that specification of the electric field ( normal derivative of the potential ) everywhere on the surface ( corresponding to a given surface - charge density ) also defines a unique problem .
6.2 , the total time derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location ...
The other result which we wish to obtain from ( 6.70 ) is the so - called Kirchhoff representation of the field inside the volume V in terms of the values of y and its derivatives on the boundary surface S. We thus assume that there are ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
TimeVarying Fields Maxwells Equations Con
4 other sections not shown