A Point Charge in an Electric Field — Question 5

Section 22-7 · Physics pages 3600–3601

Question 5 Integrating a nonuniform field avoids treating acceleration as constant A positive particle moves along x from 0 to L in the static field Ex(x) = E0(1 + x/L), with E0, L > 0. Its initial speed is v0 and its mass and charge are m and q. Ignore other forces. x Ex L Axes and labels specify the model; the sketch is schematic. (a) Use the work-energy theorem to find its speed at L. (b) Compare with approximating the field everywhere by its initial value E0. Find the error in the predicted kinetic-energy gain.
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Question 5 - Solution Integrating a nonuniform field avoids treating acceleration as constant x Ex L (a) Method and calculation W = q ∫L 0 E0(1 + x/L) dx = 3 2qE0L. 1 2m(v2 L −v2 0) = 3 2qE0L ⇒vL = √ v2 0 + 3qE0L/m. (b) Interpretation and further calculation ∆Kconst = qE0L, ∆Kexact = 3 2qE0L. ∆Kexact −∆Kconst ∆Kexact = 1/3. The average field along this straight path is 3E0/2, not its value at the start. Physical check The work integral remains valid even though the acceleration changes continuously with position.

Question 5

Integrating a nonuniform field avoids treating acceleration as constant

A positive particle moves along x from 0 to L in the static field Ex(x)=E0(1+x/L)E_x(x)=E_0(1+x/L), with E0,L>0E_0,L>0. Its initial speed is v0v_0 and its mass and charge are m and q. Ignore other forces.

Diagram shown in the original SVG worksheet.

  1. Use the work-energy theorem to find its speed at L.

  2. Compare with approximating the field everywhere by its initial value E0E_0. Find the error in the predicted kinetic-energy gain.

Question 5 - Solution

Integrating a nonuniform field avoids treating acceleration as constant

Diagram shown in the original SVG worksheet.

(a) Method and calculation

W=q∫0LE0(1+x/L)dx=32qE0L.W=q\int_0^LE_0(1+x/L)\,dx=\tfrac32qE_0L.12m(vL2−v02)=32qE0L⇒vL=v02+3qE0L/m.\tfrac12m(v_L^2-v_0^2)=\tfrac32qE_0L\Rightarrow v_L=\sqrt{v_0^2+3qE_0L/m}.

(b) Interpretation and further calculation

ΔKconst=qE0L,ΔKexact=32qE0L.\Delta K_{\mathrm{const}}=qE_0L,\quad\Delta K_{\mathrm{exact}}=\tfrac32qE_0L.ΔKexact−ΔKconstΔKexact=1/3.\frac{\Delta K_{\mathrm{exact}}-\Delta K_{\mathrm{const}}}{\Delta K_{\mathrm{exact}}}=1/3.The average field along this straight path is 3E0/23E_0/2, not its value at the start.

Physical check

The work integral remains valid even though the acceleration changes continuously with position.