The Electric Field Due to a Charged Disk — Question 3

Section 22-6 · Physics pages 3576–3577

Question 3 The infinite-sheet approximation is restricted by height relative to disk radius For a uniform disk, use E(z) = Es[1 −z/ √ z2 + R2] with Es = 2πkσ. Treat Es as the infinite-sheet approximation above the disk. z R P Schematic; labels, not drawing lengths, specify the data. (a) Find the maximum z/R for the disk field to differ from Es by at most 5 percent of Es. (b) Find the minimum disk radius needed at a height of 2.00 mm. Explain whether increasing density helps meet this relative-error criterion.
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Question 3 - Solution The infinite-sheet approximation is restricted by height relative to disk radius z R P (a) Method and calculation Es −E Es = z √ z2 + R2 ≤.0500. z/R ≤ .0500 √ 1 −.05002 ≈.0500626. (b) Interpretation and further calculation R ≥(.00200) √ 1 −.05002 .0500 ≈.0399500 m. relative error is independent of σ. Changing density scales the exact and approximate fields together; extending the radius reduces the geometric error. Physical check This bound concerns the symmetry axis; near the edge a small height alone does not ensure the same approximation.

Question 3

The infinite-sheet approximation is restricted by height relative to disk radius

For a uniform disk, use E(z)=Es[1−z/z2+R2]E(z)=E_s[1-z/\sqrt{z^2+R^2}] with Es=2πkσE_s=2\pi k\sigma. Treat EsE_s as the infinite-sheet approximation above the disk.

Diagram shown in the original SVG worksheet.

  1. Find the maximum z/Rz/R for the disk field to differ from EsE_s by at most 5 percent of EsE_s.

  2. Find the minimum disk radius needed at a height of 2.00 mm. Explain whether increasing density helps meet this relative-error criterion.

Question 3 - Solution

The infinite-sheet approximation is restricted by height relative to disk radius

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Es−EEs=zz2+R2≤.0500.\frac{E_s-E}{E_s}=\frac z{\sqrt{z^2+R^2}}\le.0500.z/R≤.05001−.05002≈.0500626.z/R\le\frac{.0500}{\sqrt{1-.0500^2}}\approx.0500626.

(b) Interpretation and further calculation

R≥(.00200)1−.05002.0500≈.0399500m.R\ge(.00200)\frac{\sqrt{1-.0500^2}}{.0500}\approx.0399500\,\mathrm m.relative error is independent of σ.\text{relative error is independent of }\sigma.Changing density scales the exact and approximate fields together; extending the radius reduces the geometric error.

Physical check

This bound concerns the symmetry axis; near the edge a small height alone does not ensure the same approximation.