Diamagnetism — Question 5

Section 32-8 · Physics pages 5320–5321

Question 5 A local minimum of field magnitude gives a diamagnetic restoring force A bead of mass m, volume V, and weak susceptibility chi less than zero is constrained to move along x. Near x=0 the applied field obeys B2 = B2 0 + ax2 with a positive. Ignore gravity along x. Use U = −χV B2/(2µ0). x B2 Schematic; labels, not drawing lengths, specify the data. (a) Find the restoring force and small-oscillation angular frequency. (b) Find the energy above the minimum at amplitude A and the maximum speed.
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Question 5 - Solution A local minimum of field magnitude gives a diamagnetic restoring force x B2 (a) Method and calculation U −U(0) = |χ|V a 2µ0 x2, Fx = −|χ|V a µ0 x . m¨x + |χ|V a µ0 x = 0 ⇒ω = √ |χ|V a µ0m . (b) Interpretation and further calculation Eosc = |χ|V aA2 2µ0 . 1 2mv2 max = Eosc ⇒vmax = ωA . Physical check The result establishes stability only along the constrained coordinate; transverse stability requires the full field geometry.

Question 5

A local minimum of field magnitude gives a diamagnetic restoring force

A bead of mass m, volume V, and weak susceptibility chi less than zero is constrained to move along x. Near x=0 the applied field obeys B2=B02+ax2B^2=B_0^2+ax^2 with a positive. Ignore gravity along x. Use U=−χVB2/(2μ0)U=-\chi VB^2/(2\mu_0).

Diagram shown in the original SVG worksheet.

  1. Find the restoring force and small-oscillation angular frequency.

  2. Find the energy above the minimum at amplitude A and the maximum speed.

Question 5 - Solution

A local minimum of field magnitude gives a diamagnetic restoring force

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U−U(0)=|χ|Va2μ0x2,Fx=−|χ|Vaμ0x.U-U(0)=\frac{|\chi|Va}{2\mu_0}x^2,\quad\boxed{F_x=-\frac{|\chi|Va}{\mu_0}x}.mẍ+|χ|Vaμ0x=0⇒ω=|χ|Vaμ0m.m\ddot x+\frac{|\chi|Va}{\mu_0}x=0\Rightarrow\boxed{\omega=\sqrt{\frac{|\chi|Va}{\mu_0m}}}.

(b) Interpretation and further calculation

Eosc=|χ|VaA22μ0.\boxed{E_{\mathrm{osc}}=\frac{|\chi|VaA^2}{2\mu_0}}.12mvmax⁡2=Eosc⇒vmax=ωA.\tfrac12mv_{\max}^2=E_{\mathrm{osc}}\Rightarrow\boxed{v_{\max}=\omega A}.

Physical check

The result establishes stability only along the constrained coordinate; transverse stability requires the full field geometry.