Electricity and Magnetism · Problem 10.6

MAGNETIC FIELDS IN MATTER — Edward Purcell & David Morin

Physics — E&M · quadrupole-tensor

Problem

You should see the quadrupole tensor at least once in your life, so here it is. Calculate the general form of the quadrupole tensor by writing the RR in Eq. (10.5) in Cartesian form as R=(x1−x1′)2+(x2−x2′)2+(x3−x3′)2,R = \sqrt{(x_1 - x_1')^2 + (x_2 - x_2')^2 + (x_3 - x_3')^2}, and then performing a Taylor expansion as we did in Section 10.2. (It's a little cleaner to work with x1,x2,x3x_1, x_2, x_3 instead of x,y,zx, y, z.) Your goal is to write the 1/r31/r^3 part of the potential in a form that has all of its dependence on the primed coordinates collected into a matrix. (By analogy, the 1/r21/r^2 part of the potential in Eq. (10.12) has all of its dependence on the primed coordinates collected into the vector p\mathbf{p} given by Eq. (10.13).)

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