The Electric Field Due to a Line of Charge — Question 3

Section 22-5 · Physics pages 3556–3557

Question 3 Near an endpoint a uniformly charged rod cannot be replaced by its center charge A uniform rod occupies 0 ≤x ≤L with L = .400 m and λ = 3.00 nC/m. Observe at x = −s, where s = .200 m. Use k = 8.99 × 109 N m2/C2. P 0 L s Schematic; labels, not drawing lengths, specify the data. (a) Integrate the axial field and evaluate it. (b) Compare with placing the total rod charge at its midpoint; report the fractional underestimate relative to the exact magnitude.
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Question 3 - Solution Near an endpoint a uniformly charged rod cannot be replaced by its center charge P 0 L s (a) Method and calculation Ex = −kλ ∫L 0 dx (s + x)2 = −kλ (1 s − 1 s + L ) . Ex = −89.9 N/C, Q = λL = 1.20 nC. (b) Interpretation and further calculation Ecenter = − kQ (s + L/2)2 = −67.425 N/C. |Eexact| −|Ecenter| |Eexact| = .250. The closer part of the rod contributes disproportionately because the kernel varies as inverse distance squared. Physical check The field points left, away from every positive source element.

Question 3

Near an endpoint a uniformly charged rod cannot be replaced by its center charge

A uniform rod occupies 0≤x≤L0\le x\le L with L=.400L=.400 m and λ=3.00\lambda=3.00 nC/m. Observe at x=−sx=-s, where s=.200s=.200 m. Use k=8.99×109k=8.99\times10^9 N m2^2/C2^2.

Diagram shown in the original SVG worksheet.

  1. Integrate the axial field and evaluate it.

  2. Compare with placing the total rod charge at its midpoint; report the fractional underestimate relative to the exact magnitude.

Question 3 - Solution

Near an endpoint a uniformly charged rod cannot be replaced by its center charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=−kλ∫0Ldx(s+x)2=−kλ(1s−1s+L).E_x=-k\lambda\int_0^L\frac{dx}{(s+x)^2}=-k\lambda\left(\frac1s-\frac1{s+L}\right).Ex=−89.9N/C,Q=λL=1.20nC.E_x=-89.9\,\mathrm{N/C},\quad Q=\lambda L=1.20\,\mathrm{nC}.

(b) Interpretation and further calculation

Ecenter=−kQ(s+L/2)2=−67.425N/C.E_{\mathrm{center}}=-\frac{kQ}{(s+L/2)^2}=-67.425\,\mathrm{N/C}.|Eexact|−|Ecenter||Eexact|=.250.\frac{|E_{\mathrm{exact}}|-|E_{\mathrm{center}}|}{|E_{\mathrm{exact}}|}=.250.The closer part of the rod contributes disproportionately because the kernel varies as inverse distance squared.

Physical check

The field points left, away from every positive source element.