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A point charge q moves with a non-relativistic velocity v = const. Applying the theorem for the

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A point charge q moves with a non-relativistic velocity v = const. Applying the theorem for the circulation of the vector I4 around the dotted circle shown in Fig. 3.97, find H at the point A as a function of a radius vector r and velocity v of the charge.


A
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A

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We use Maxwells equations in the form a BdrEds t when the conduction current vanishes at the ...View the full answer


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