Magnets — Question 10

Section 32-5 · Physics pages 5270–5271

Question 10 Translation and rotation give the same total work along two paths A permanent dipole m is moved quasistatically from field magnitude B1 to B2. The local field direction is +x throughout the constrained path. Initially the moment is parallel; finally it is antiparallel. Neglect dissipation. parallel, B1 parallel, B2 antiparallel, B1 antiparallel, B2 Schematic; labels, not drawing lengths, specify the data. (a) Compute total external work by first translating while parallel and then rotating at B2. (b) Compute it by first rotating at B1 and then translating while antiparallel. Compare the totals.
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Question 10 - Solution Translation and rotation give the same total work along two paths parallel, B1 parallel, B2 antiparallel, B1 antiparallel, B2 (a) Method and calculation Wtranslate,A = −m(B2 −B1), Wrotate,A = 2mB2. WA = m(B1 + B2) . (b) Interpretation and further calculation Wrotate,B = 2mB1, Wtranslate,B = m(B2 −B1). WB = m(B1 + B2) = Uf −Ui = WA . Physical check Individual work contributions depend on the path, but conservative quasistatic total work depends only on the endpoints.

Question 10

Translation and rotation give the same total work along two paths

A permanent dipole m is moved quasistatically from field magnitude B1 to B2. The local field direction is +x throughout the constrained path. Initially the moment is parallel; finally it is antiparallel. Neglect dissipation.

Diagram shown in the original SVG worksheet.

  1. Compute total external work by first translating while parallel and then rotating at B2.

  2. Compute it by first rotating at B1 and then translating while antiparallel. Compare the totals.

Question 10 - Solution

Translation and rotation give the same total work along two paths

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Wtranslate,A=−m(B2−B1),Wrotate,A=2mB2.W_{\mathrm{translate,A}}=-m(B_2-B_1),\quad W_{\mathrm{rotate,A}}=2mB_2.WA=m(B1+B2).\boxed{W_A=m(B_1+B_2)}.

(b) Interpretation and further calculation

Wrotate,B=2mB1,Wtranslate,B=m(B2−B1).W_{\mathrm{rotate,B}}=2mB_1,\quad W_{\mathrm{translate,B}}=m(B_2-B_1).WB=m(B1+B2)=Uf−Ui=WA.\boxed{W_B=m(B_1+B_2)=U_f-U_i=W_A}.

Physical check

Individual work contributions depend on the path, but conservative quasistatic total work depends only on the endpoints.