Ferromagnetism — Question 3

Section 32-10 · Physics pages 5356–5357

Question 3 A rectangular magnetization loop converts its area into heat An ideal hysteresis cycle switches abruptly between M=-Ms and M=+Ms at internal fields +Hc and -Hc, respectively. Outside the switches M is constant. Use the loss per unit volume w = H H dB, with B = µ0(H + M). H M Hc Ms Schematic; labels, not drawing lengths, specify the data. (a) Derive w from the two switching events. (b) Find average loss power for sample volume V cycled at frequency f, and evaluate it for Ms = 8.0 × 105 A/m, Hc = 100 A/m, V = 2.0 × 10−5 cubic meters, and f=50 Hz. Use µ0 = 4π × 10−7 H/m.
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Question 3 - Solution A rectangular magnetization loop converts its area into heat H M Hc Ms (a) Method and calculation w = µ0 I H dH + µ0 I H dM = µ0 I H dM. w = µ0[(Hc)(2Ms) + (−Hc)(−2Ms)] = 4µ0HcMs . (b) Interpretation and further calculation P = fV w = 4µ0fV HcMs . w = 402.124 J/m3, P = 0.4021 W . Physical check This quasistatic loop-area loss excludes additional eddy-current and dynamic losses.

Question 3

A rectangular magnetization loop converts its area into heat

An ideal hysteresis cycle switches abruptly between M=-Ms and M=+Ms at internal fields +Hc and -Hc, respectively. Outside the switches M is constant. Use the loss per unit volume w=∮HdBw=\oint H\,dB, with B=μ0(H+M)B=\mu_0(H+M).

Diagram shown in the original SVG worksheet.

  1. Derive w from the two switching events.

  2. Find average loss power for sample volume V cycled at frequency f, and evaluate it for Ms=8.0×105M_s=8.0\times10^5 A/m, Hc=100H_c=100 A/m, V=2.0×10−5V=2.0\times10^{-5} cubic meters, and f=50 Hz. Use μ0=4π×10−7\mu_0=4\pi\times10^{-7} H/m.

Question 3 - Solution

A rectangular magnetization loop converts its area into heat

Diagram shown in the original SVG worksheet.

(a) Method and calculation

w=μ0∮HdH+μ0∮HdM=μ0∮HdM.w=\mu_0\oint H\,dH+\mu_0\oint H\,dM=\mu_0\oint H\,dM.w=μ0[(Hc)(2Ms)+(−Hc)(−2Ms)]=4μ0HcMs.w=\mu_0[(H_c)(2M_s)+(-H_c)(-2M_s)]=\boxed{4\mu_0H_cM_s}.

(b) Interpretation and further calculation

P=fVw=4μ0fVHcMs.\boxed{P=fVw=4\mu_0fVH_cM_s}.w=402.124J/m3,P=0.4021W.w=402.124\,\mathrm{J/m^3},\qquad\boxed{P=0.4021\,\mathrm W}.

Physical check

This quasistatic loop-area loss excludes additional eddy-current and dynamic losses.