Two Experiments — Question 2

Section 30-1 · Physics pages 4754–4755

Question 2 Doubling the passage speed changes pulse height but not signed transferred charge A moving magnet produces pickup linkage Λ(x) between fixed positions x1 and x2. One run uses speed v and another uses speed 2v along the same path. For this calibrated experiment, use signed flux linkage Λ = NΦ, E = −dΛ/dt and i = E/R; neglect pickup self-inductance. S N v pickup coil Schematic; labels, not drawing lengths, specify the data. (a) Compare the emf at the same position and the passage duration. (b) Compare the signed charge transported between the two endpoint positions.
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Question 2 - Solution Doubling the passage speed changes pulse height but not signed transferred charge S N v pickup coil (a) Method and calculation E = −dΛ dx v ⇒E2v(x) = 2Ev(x) . ∆t = (x2 −x1)/v ⇒∆t2v = ∆tv/2. (b) Interpretation and further calculation Q = ∫ i dt = −1 R ∫ dΛ = −Λ(x2) −Λ(x1) R . Q2v = Qv . Physical check A faster pulse is taller and shorter. The invariance concerns signed charge between the same linkage endpoints, not dissipated heat.

Question 2

Doubling the passage speed changes pulse height but not signed transferred charge

A moving magnet produces pickup linkage Λ(x)\Lambda(x) between fixed positions x1 and x2. One run uses speed v and another uses speed 2v along the same path. 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. Compare the emf at the same position and the passage duration.

  2. Compare the signed charge transported between the two endpoint positions.

Question 2 - Solution

Doubling the passage speed changes pulse height but not signed transferred charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℰ=−dΛdxv⇒ℰ2v(x)=2ℰv(x).\mathcal E=-\frac{d\Lambda}{dx}v\Rightarrow\boxed{\mathcal E_{2v}(x)=2\mathcal E_v(x)}.Δt=(x2−x1)/v⇒Δt2v=Δtv/2.\Delta t=(x_2-x_1)/v\Rightarrow\Delta t_{2v}=\Delta t_v/2.

(b) Interpretation and further calculation

Q=∫idt=−1R∫dΛ=−Λ(x2)−Λ(x1)R.Q=\int i\,dt=-\frac1R\int d\Lambda=-\frac{\Lambda(x_2)-\Lambda(x_1)}R.Q2v=Qv.\boxed{Q_{2v}=Q_v}.

Physical check

A faster pulse is taller and shorter. The invariance concerns signed charge between the same linkage endpoints, not dissipated heat.