Diamagnetism — Question 8

Section 32-8 · Physics pages 5326–5327

Question 8 A perfectly diamagnetic sphere needs a demagnetizing-field correction An ideal sphere excludes magnetic induction from its interior: B=0. In a uniform applied field Ha its internal field obeys H = Ha −M/3. Use B = µ0(H + M). Ignore penetration depth. B = 0 Ha M Schematic; labels, not drawing lengths, specify the data. (a) Find internal H, magnetization M, and apparent susceptibility M/Ha. (b) For sphere radius a, find its total dipole moment and explain why apparent susceptibility differs from intrinsic M/H.
Show solutionHide solution
Question 8 - Solution A perfectly diamagnetic sphere needs a demagnetizing-field correction B = 0 Ha M (a) Method and calculation B = 0 ⇒M = −H, H = Ha + H/3. H = 3 2Ha, M = −3 2Ha . (b) Interpretation and further calculation χapp = M/Ha = −3/2, χint = M/H = −1 . m = 4πa3 3 M = −2πa3Ha . Physical check This ideal complete-exclusion limit is distinct from the tiny negative susceptibility of ordinary weak diamagnets.

Question 8

A perfectly diamagnetic sphere needs a demagnetizing-field correction

An ideal sphere excludes magnetic induction from its interior: B=0. In a uniform applied field Ha its internal field obeys H=Ha−M/3H=H_a-M/3. Use B=μ0(H+M)B=\mu_0(H+M). Ignore penetration depth.

Diagram shown in the original SVG worksheet.

  1. Find internal H, magnetization M, and apparent susceptibility M/Ha.

  2. For sphere radius a, find its total dipole moment and explain why apparent susceptibility differs from intrinsic M/H.

Question 8 - Solution

A perfectly diamagnetic sphere needs a demagnetizing-field correction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

B=0⇒M=−H,H=Ha+H/3.B=0\Rightarrow M=-H,\quad H=H_a+H/3.H=32Ha,M=−32Ha.\boxed{H=\tfrac32H_a,\quad M=-\tfrac32H_a}.

(b) Interpretation and further calculation

χapp=M/Ha=−3/2,χint=M/H=−1.\boxed{\chi_{\mathrm{app}}=M/H_a=-3/2,\quad\chi_{\mathrm{int}}=M/H=-1}.m=4πa33M=−2πa3Ha.\boxed{m=\frac{4\pi a^3}{3}M=-2\pi a^3H_a}.

Physical check

This ideal complete-exclusion limit is distinct from the tiny negative susceptibility of ordinary weak diamagnets.