Equipotential Surfaces — Question 5

Section 24-3 · Physics pages 3840–3841

Question 5 Equal endpoint potential permits speed changes during the intervening trip Along an ideal constrained path of length L, V (s) = V0 + B sin(2πs/L) with B > 0. A positive particle q starts at s=0 with kinetic energy K0 = 2qB. The guide does no work. s V L Axes and labels specify the model; the sketch is schematic. (a) Find kinetic energy along the path and at s=L. (b) Find the minimum and maximum speeds for mass m and explain why zero net electric work does not mean zero force throughout.
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Question 5 - Solution Equal endpoint potential permits speed changes during the intervening trip s V L (a) Method and calculation K(s) = K0 −q[V (s) −V0] = qB[2 −sin(2πs/L)]. K(L) = K0, W0→L = 0. (b) Interpretation and further calculation vmin = √ 2qB/m, vmax = √ 6qB/m. Fs = −qdV ds = −2πqB L cos(2πs/L). Physical check Equal endpoint voltages fix net work; only motion entirely on one equipotential makes the electric work vanish on every subsegment.

Question 5

Equal endpoint potential permits speed changes during the intervening trip

Along an ideal constrained path of length L, V(s)=V0+Bsin⁡(2πs/L)V(s)=V_0+B\sin(2\pi s/L) with B>0B>0. A positive particle q starts at s=0 with kinetic energy K0=2qBK_0=2qB. The guide does no work.

Diagram shown in the original SVG worksheet.

  1. Find kinetic energy along the path and at s=L.

  2. Find the minimum and maximum speeds for mass m and explain why zero net electric work does not mean zero force throughout.

Question 5 - Solution

Equal endpoint potential permits speed changes during the intervening trip

Diagram shown in the original SVG worksheet.

(a) Method and calculation

K(s)=K0−q[V(s)−V0]=qB[2−sin⁡(2πs/L)].K(s)=K_0-q[V(s)-V_0]=qB[2-\sin(2\pi s/L)].K(L)=K0,W0→L=0.K(L)=K_0,\quad W_{0\to L}=0.

(b) Interpretation and further calculation

vmin=2qB/m,vmax=6qB/m.v_{\min}=\sqrt{2qB/m},\quad v_{\max}=\sqrt{6qB/m}.Fs=−qdVds=−2πqBLcos⁡(2πs/L).F_s=-q\frac{dV}{ds}=-\frac{2\pi qB}{L}\cos(2\pi s/L).

Physical check

Equal endpoint voltages fix net work; only motion entirely on one equipotential makes the electric work vanish on every subsegment.