Diamagnetism — Question 3

Section 32-8 · Physics pages 5316–5317

Question 3 A diamagnetic bead moves toward lower field magnitude A small isotropic bead has volume V and weak susceptibility chi less than zero. Neglect its disturbance of the applied field. Its effective mechanical potential is U = −χV B2/(2µ0). Along x, B2 = B2 0 + ax, with a positive. x F B2 increases to the right Schematic; labels, not drawing lengths, specify the data. (a) Find the magnetic force and the work it does when the bead moves a distance d in +x. (b) Find the quasistatic external work for that displacement and the dependence on the sign of B.
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Question 3 - Solution A diamagnetic bead moves toward lower field magnitude x F B2 increases to the right (a) Method and calculation Fx = −∂xU = χV a 2µ0 < 0 . Wmag = Fxd = χV ad 2µ0 < 0 . (b) Interpretation and further calculation Wext = ∆U = −Wmag = |χ|V ad 2µ0 > 0 . B →−B ⇒B2 unchanged ⇒Fx unchanged . Physical check The gradient of field magnitude squared sets the force; reversing the field direction alone does not reverse a diamagnetic force.

Question 3

A diamagnetic bead moves toward lower field magnitude

A small isotropic bead has volume V and weak susceptibility chi less than zero. Neglect its disturbance of the applied field. Its effective mechanical potential is U=−χVB2/(2μ0)U=-\chi VB^2/(2\mu_0). Along x, B2=B02+axB^2=B_0^2+ax, with a positive.

Diagram shown in the original SVG worksheet.

  1. Find the magnetic force and the work it does when the bead moves a distance d in +x.

  2. Find the quasistatic external work for that displacement and the dependence on the sign of B.

Question 3 - Solution

A diamagnetic bead moves toward lower field magnitude

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Fx=−∂xU=χVa2μ0<0.F_x=-\partial_xU=\boxed{\frac{\chi Va}{2\mu_0}<0}.Wmag=Fxd=χVad2μ0<0.\boxed{W_{\mathrm{mag}}=F_xd=\frac{\chi Vad}{2\mu_0}<0}.

(b) Interpretation and further calculation

Wext=ΔU=−Wmag=|χ|Vad2μ0>0.W_{\mathrm{ext}}=\Delta U=-W_{\mathrm{mag}}=\boxed{\frac{|\chi|Vad}{2\mu_0}>0}.B→−B⇒B2 unchanged⇒Fx unchanged.B\to-B\Rightarrow B^2\text{ unchanged}\Rightarrow\boxed{F_x\text{ unchanged}}.

Physical check

The gradient of field magnitude squared sets the force; reversing the field direction alone does not reverse a diamagnetic force.