The Electric Field Due to a Charged Disk — Question 4

Section 22-6 · Physics pages 3578–3579

Question 4 A far-away disk approaches a point charge from below A uniformly charged disk has total charge Q and radius R. On its positive axis, E = 2kQ[1 −z/ √ z2 + R2]/R2. Compare with Ep = kQ/z2. z R P Schematic; labels, not drawing lengths, specify the data. (a) Find the exact ratio E/Ep and evaluate it at z = 5R. (b) Use (1 + u)−1/2 = 1 −u/2 + 3u2/8 + O(u3) to find the leading relative correction.
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Question 4 - Solution A far-away disk approaches a point charge from below z R P (a) Method and calculation E Ep = 2z2 R2 ( 1 − z √ z2 + R2 ) . z = 5R : E/Ep = 50(1 −5/ √ 26) ≈.970966. (b) Interpretation and further calculation u = R2/z2 : 1 −(1 + u)−1/2 = u/2 −3u2/8 + O(u3). E/Ep = 1 −3R2 4z2 + O(R4/z4). The point-charge estimate is too large because distributed charge has greater distance and smaller axial projection than charge concentrated at the center. Physical check The expansion must retain one extra term before division by u to capture the first field correction.

Question 4

A far-away disk approaches a point charge from below

A uniformly charged disk has total charge Q and radius R. On its positive axis, E=2kQ[1−z/z2+R2]/R2E=2kQ[1-z/\sqrt{z^2+R^2}]/R^2. Compare with Ep=kQ/z2E_p=kQ/z^2.

Diagram shown in the original SVG worksheet.

  1. Find the exact ratio E/EpE/E_p and evaluate it at z=5Rz=5R.

  2. Use (1+u)−1/2=1−u/2+3u2/8+O(u3)(1+u)^{-1/2}=1-u/2+3u^2/8+O(u^3) to find the leading relative correction.

Question 4 - Solution

A far-away disk approaches a point charge from below

Diagram shown in the original SVG worksheet.

(a) Method and calculation

EEp=2z2R2(1−zz2+R2).\frac E{E_p}=\frac{2z^2}{R^2}\left(1-\frac z{\sqrt{z^2+R^2}}\right).z=5R:E/Ep=50(1−5/26)≈.970966.z=5R:\quad E/E_p=50(1-5/\sqrt{26})\approx.970966.

(b) Interpretation and further calculation

u=R2/z2:1−(1+u)−1/2=u/2−3u2/8+O(u3).u=R^2/z^2:\quad1-(1+u)^{-1/2}=u/2-3u^2/8+O(u^3).E/Ep=1−3R24z2+O(R4/z4).E/E_p=1-\frac{3R^2}{4z^2}+O(R^4/z^4).The point-charge estimate is too large because distributed charge has greater distance and smaller axial projection than charge concentrated at the center.

Physical check

The expansion must retain one extra term before division by uu to capture the first field correction.