In Prob. 6.4, you calculated the force on a dipole by “brute force.” Here’s a more elegant approach. First write B(r) as a Taylor expansion about the center of the loop:
where r0 is the position of the dipole and ∇0 denotes differentiation with respect to r0. Put this into the Lorentz force law (Eq. 5.16) to obtain
Or, numbering the Cartesian coordinates from 1 to 3:
where δi j is the Kronecker delta (Prob. 3.52).
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