Two Experiments — Question 9

Section 30-1 · Physics pages 4768–4769

Question 9 A symmetric magnet passage has zero net charge but nonzero heating A magnet traverses a pickup so its linkage starts at zero, rises linearly to Lambda0 in time T and falls linearly to zero in another time T. Pickup resistance is R. For this calibrated experiment, use signed flux linkage Λ = NΦ, E = −dΛ/dt and i = E/R; neglect pickup self-inductance. t Λ Schematic; labels, not drawing lengths, specify the data. (a) Find current and total signed charge. (b) Find the heat dissipated over the full passage and its dependence on T.
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Question 9 - Solution A symmetric magnet passage has zero net charge but nonzero heating t Λ (a) Method and calculation irise = −Λ0 RT , ifall = + Λ0 RT . Q = iriseT + ifallT = 0 . (b) Interpretation and further calculation H = ∫2T 0 i2Rdt = 2T Λ2 0 RT 2 . H = 2Λ2 0 RT ∝T −1 . Physical check Signed charge can cancel while heat, proportional to current squared, accumulates in both halves.

Question 9

A symmetric magnet passage has zero net charge but nonzero heating

A magnet traverses a pickup so its linkage starts at zero, rises linearly to Lambda0 in time T and falls linearly to zero in another time T. Pickup resistance is R. For this calibrated experiment, use signed flux linkage Λ=NΦ\Lambda=N\Phi, ℰ=−dΛ/dt\mathcal E=-d\Lambda/dt and i=ℰ/Ri=\mathcal E/R; neglect pickup self-inductance.

Diagram shown in the original SVG worksheet.

  1. Find current and total signed charge.

  2. Find the heat dissipated over the full passage and its dependence on T.

Question 9 - Solution

A symmetric magnet passage has zero net charge but nonzero heating

Diagram shown in the original SVG worksheet.

(a) Method and calculation

irise=−Λ0RT,ifall=+Λ0RT.i_{\mathrm{rise}}=-\frac{\Lambda_0}{RT},\quad i_{\mathrm{fall}}=+\frac{\Lambda_0}{RT}.Q=iriseT+ifallT=0.\boxed{Q=i_{\mathrm{rise}}T+i_{\mathrm{fall}}T=0}.

(b) Interpretation and further calculation

H=∫02Ti2Rdt=2TΛ02RT2.H=\int_0^{2T}i^2Rdt=2T\frac{\Lambda_0^2}{RT^2}.H=2Λ02RT∝T−1.\boxed{H=\frac{2\Lambda_0^2}{RT}\propto T^{-1}}.

Physical check

Signed charge can cancel while heat, proportional to current squared, accumulates in both halves.