The Electric Field Due to a Line of Charge — Question 2

Section 22-5 · Physics pages 3554–3555

Question 2 A long-line approximation requires enough charged length on both sides For a uniform rod of half-length L, Ef = 2kλL/[y √ L2 + y2] at its perpendicular bisector. The infinite-line approximation is E∞= 2kλ/y. Define the fractional deficit relative to the infinite-line value. −L L P Schematic; labels, not drawing lengths, specify the data. (a) Derive the deficit and find the minimum L/y for it to be no greater than 1 percent. (b) Evaluate the deficit when L = 3y and state whether increasing line density improves the approximation.
Show solutionHide solution
Question 2 - Solution A long-line approximation requires enough charged length on both sides −L L P (a) Method and calculation δ = E∞−Ef E∞ = 1 − L √ L2 + y2 . δ ≤.01 ⇒L/y ≥ .99 √ 1 −.992 ≈7.01792. (b) Interpretation and further calculation L = 3y : δ = 1 −3/ √ 10 ≈.0513167. Ef/E∞is independent of λ. More charge scales both fields equally; only the length-to-distance ratio controls this relative geometric error. Physical check L is the half-length; the required full length is approximately 14.0358y.

Question 2

A long-line approximation requires enough charged length on both sides

For a uniform rod of half-length L, Ef=2kλL/[yL2+y2]E_f=2k\lambda L/[y\sqrt{L^2+y^2}] at its perpendicular bisector. The infinite-line approximation is E∞=2kλ/yE_\infty=2k\lambda/y. Define the fractional deficit relative to the infinite-line value.

Diagram shown in the original SVG worksheet.

  1. Derive the deficit and find the minimum L/yL/y for it to be no greater than 1 percent.

  2. Evaluate the deficit when L=3yL=3y and state whether increasing line density improves the approximation.

Question 2 - Solution

A long-line approximation requires enough charged length on both sides

Diagram shown in the original SVG worksheet.

(a) Method and calculation

δ=E∞−EfE∞=1−LL2+y2.\delta=\frac{E_\infty-E_f}{E_\infty}=1-\frac{L}{\sqrt{L^2+y^2}}.δ≤.01⇒L/y≥.991−.992≈7.01792.\delta\le.01\Rightarrow L/y\ge\frac{.99}{\sqrt{1-.99^2}}\approx7.01792.

(b) Interpretation and further calculation

L=3y:δ=1−3/10≈.0513167.L=3y:\quad\delta=1-3/\sqrt{10}\approx.0513167.Ef/E∞is independent of λ.E_f/E_\infty\ \text{is independent of }\lambda.More charge scales both fields equally; only the length-to-distance ratio controls this relative geometric error.

Physical check

L is the half-length; the required full length is approximately 14.0358y14.0358y.