A Point Charge in an Electric Field — Question 7

Section 22-7 · Physics pages 3604–3605

Question 7 Opposite deflecting pulses restore velocity without restoring position A particle with q > 0 moves horizontally at constant speed v and has zero initial transverse velocity. It experiences +Eˆy for time τ, then −Eˆy for another τ. The field has no x component; let a = qE/m. +Ey −Ey Schematic; labels, not drawing lengths, specify the data. (a) Find the transverse displacement and velocity at the end of each interval. (b) Find the total electric work and explain how the particle can finish displaced with its original speed.
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Question 7 - Solution Opposite deflecting pulses restore velocity without restoring position +Ey −Ey (a) Method and calculation vy,1 = aτ, y1 = 1 2aτ 2. vy,2 = aτ −aτ = 0, ∆y2 = aτ 2 −1 2aτ 2 = 1 2aτ 2. (b) Interpretation and further calculation yf = aτ 2, vf = v. W1 = 1 2ma2τ 2, W2 = −1 2ma2τ 2, Wtotal = 0. Equal opposite impulses remove the transverse velocity, but the accumulated transverse displacement remains. Physical check Zero net impulse constrains final momentum, not the integral of velocity over the flight.

Question 7

Opposite deflecting pulses restore velocity without restoring position

A particle with q>0q>0 moves horizontally at constant speed v and has zero initial transverse velocity. It experiences +E𝒚̂+E\hat{\mathbf y} for time τ\tau, then −E𝒚̂-E\hat{\mathbf y} for another τ\tau. The field has no x component; let a=qE/ma=qE/m.

Diagram shown in the original SVG worksheet.

  1. Find the transverse displacement and velocity at the end of each interval.

  2. Find the total electric work and explain how the particle can finish displaced with its original speed.

Question 7 - Solution

Opposite deflecting pulses restore velocity without restoring position

Diagram shown in the original SVG worksheet.

(a) Method and calculation

vy,1=aτ,y1=12aτ2.v_{y,1}=a\tau,\quad y_1=\tfrac12a\tau^2.vy,2=aτ−aτ=0,Δy2=aτ2−12aτ2=12aτ2.v_{y,2}=a\tau-a\tau=0,\quad\Delta y_2=a\tau^2-\tfrac12a\tau^2=\tfrac12a\tau^2.

(b) Interpretation and further calculation

yf=aτ2,vf=v.y_f=a\tau^2,\quad v_f=v.W1=12ma2τ2,W2=−12ma2τ2,Wtotal=0.W_1=\tfrac12ma^2\tau^2,\quad W_2=-\tfrac12ma^2\tau^2,\quad W_{\mathrm{total}}=0.Equal opposite impulses remove the transverse velocity, but the accumulated transverse displacement remains.

Physical check

Zero net impulse constrains final momentum, not the integral of velocity over the flight.