A Point Charge in an Electric Field — Question 6

Section 22-7 · Physics pages 3602–3603

Question 6 A ramped field gives the same impulse as its mean but a different displacement A particle starts from rest in a spatially uniform field Ex(t) = E0t/τ for 0 ≤t ≤τ. Its mass is m and charge is q > 0. Other forces are negligible. t Ex τ Axes and labels specify the model; the sketch is schematic. (a) Integrate the acceleration to find velocity and displacement at the end of the pulse. (b) Compare with using the constant time-average field E0/2. Identify which final quantity is reproduced and which is not.
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Question 6 - Solution A ramped field gives the same impulse as its mean but a different displacement t Ex τ (a) Method and calculation ax(t) = qE0 mτ t, vx(t) = qE0t2 2mτ . vx(τ) = qE0τ 2m , x(τ) = qE0τ 2 6m . (b) Interpretation and further calculation ¯E = E0/2 : vavg(τ) = qE0τ 2m , xavg(τ) = qE0τ 2 4m . xavg/xexact = 3/2. Impulse depends on the time integral of force, whereas displacement also depends on when the acceleration occurs. Physical check Later acceleration contributes less time to displacement than earlier acceleration of the same impulse.

Question 6

A ramped field gives the same impulse as its mean but a different displacement

A particle starts from rest in a spatially uniform field Ex(t)=E0t/τE_x(t)=E_0t/\tau for 0≤t≤τ0\le t\le\tau. Its mass is m and charge is q>0q>0. Other forces are negligible.

Diagram shown in the original SVG worksheet.

  1. Integrate the acceleration to find velocity and displacement at the end of the pulse.

  2. Compare with using the constant time-average field E0/2E_0/2. Identify which final quantity is reproduced and which is not.

Question 6 - Solution

A ramped field gives the same impulse as its mean but a different displacement

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ax(t)=qE0mτt,vx(t)=qE0t22mτ.a_x(t)=\frac{qE_0}{m\tau}t,\quad v_x(t)=\frac{qE_0t^2}{2m\tau}.vx(τ)=qE0τ2m,x(τ)=qE0τ26m.v_x(\tau)=\frac{qE_0\tau}{2m},\quad x(\tau)=\frac{qE_0\tau^2}{6m}.

(b) Interpretation and further calculation

E‾=E0/2:vavg(τ)=qE0τ2m,xavg(τ)=qE0τ24m.\bar E=E_0/2:\quad v_{\mathrm{avg}}(\tau)=\frac{qE_0\tau}{2m},\quad x_{\mathrm{avg}}(\tau)=\frac{qE_0\tau^2}{4m}.xavg/xexact=3/2.x_{\mathrm{avg}}/x_{\mathrm{exact}}=3/2.Impulse depends on the time integral of force, whereas displacement also depends on when the acceleration occurs.

Physical check

Later acceleration contributes less time to displacement than earlier acceleration of the same impulse.