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... the circulating currents inside atoms or molecules. The total vector potential
due to all currents is 1 Cl(v'\ rPr' 1 fl(f'\fflr' = 1 J(x)d* +1 Jfl(x)dx cJ |x — x I cJ |x — x
I We use a small a for the microscopic vector potential, just as we used e for the ...
Combining the first term in (5.79) with the conduction-current term in (5.76), we
can write the vector potential as = 1 ri(x') + cV x M(x')^, cJ |x — x'l We see that the
magnetization contributes to the vector potential as an effective current density ...
Then the vector potential is A(x) = — f J(x') , e ' ' A d3x' (9.7) cr J In the
approximation that r > d and d < A it is legitimate to expand the exponential and
its denominator as a power series in (n • x'). Then we have / n•x \ V ~r~J r c,r«rr , 1
/2 2/fc ,2\, .
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Introduction to Electrostatics
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