Ferromagnetism — Question 8

Section 32-10 · Physics pages 5366–5367

Question 8 An air gap moves a permanent magnet away from its zero-field remanence A closed permanent-magnet circuit has magnet length ell, a gap g, equal cross-sectional area throughout, and no free current. Neglect leakage and fringing. On its recoil line the magnet obeys B = Br + µ0µrecHm; the gap has Hg = B/µ0. g magnet path length ℓ Schematic; labels, not drawing lengths, specify the data. (a) Use Ampere law to find B in the gap and Hm in the magnet. (b) Find g/ell needed to reduce B to Br/2, and explain why B generally differs from Br even with no current.
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Question 8 - Solution An air gap moves a permanent magnet away from its zero-field remanence g magnet path length ℓ (a) Method and calculation Hmℓ+ Hgg = 0 ⇒Hm = −Bg µ0ℓ. B = Br −µrecBg/ℓ⇒B = Br 1 + µrecg/ℓ. (b) Interpretation and further calculation B = Br/2 ⇒g/ℓ= 1/µrec . Hm = − Brg µ0(ℓ+ µrecg)̸ = 0 (g > 0). Physical check Zero free current fixes the total circulation of H, not H at every point; the gap creates a demagnetizing operating field.

Question 8

An air gap moves a permanent magnet away from its zero-field remanence

A closed permanent-magnet circuit has magnet length ell, a gap g, equal cross-sectional area throughout, and no free current. Neglect leakage and fringing. On its recoil line the magnet obeys B=Br+μ0μrecHmB=B_r+\mu_0\mu_{\mathrm{rec}}H_m; the gap has Hg=B/μ0H_g=B/\mu_0.

Diagram shown in the original SVG worksheet.

  1. Use Ampere law to find B in the gap and Hm in the magnet.

  2. Find g/ell needed to reduce B to Br/2, and explain why B generally differs from Br even with no current.

Question 8 - Solution

An air gap moves a permanent magnet away from its zero-field remanence

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Hmℓ+Hgg=0⇒Hm=−Bgμ0ℓ.H_m\ell+H_gg=0\Rightarrow H_m=-\frac{Bg}{\mu_0\ell}.B=Br−μrecBg/ℓ⇒B=Br1+μrecg/ℓ.B=B_r-\mu_{\mathrm{rec}}Bg/\ell\Rightarrow\boxed{B=\frac{B_r}{1+\mu_{\mathrm{rec}}g/\ell}}.

(b) Interpretation and further calculation

B=Br/2⇒g/ℓ=1/μrec.B=B_r/2\Rightarrow\boxed{g/\ell=1/\mu_{\mathrm{rec}}}.Hm=−Brgμ0(ℓ+μrecg)≠0(g>0).\boxed{H_m=-\frac{B_rg}{\mu_0(\ell+\mu_{\mathrm{rec}}g)}}\ne0\quad(g>0).

Physical check

Zero free current fixes the total circulation of H, not H at every point; the gap creates a demagnetizing operating field.