Applying Gauss' Law: Cylindrical Symmetry — Question 3

Section 23-6 · Physics pages 3736–3737

Question 3 A hollow insulating cylinder begins building field only beyond its inner radius An infinite insulating tube occupies a < r < b and carries uniform fixed density ρ > 0. Its hollow core and exterior contain no charge. There are no other sources. a b Cross-section perpendicular to an infinite cylinder axis; end effects are excluded. (a) Derive the radial field in all three regions. (b) Find the radius within the charged material where the field equals half its value at b. Define C = (b2 −a2)/(2b) to simplify the algebra.
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Question 3 - Solution A hollow insulating cylinder begins building field only beyond its inner radius a b (a) Method and calculation λenc =        0, r < a, πρ(r2 −a2), a < r < b, πρ(b2 −a2), r > b. Er = λenc 2πϵ0r. (b) Interpretation and further calculation ρ 2ϵ0 ( r −a2 r ) = ρ(b2 −a2) 4ϵ0b ⇒r2 −Cr −a2 = 0. r1/2 = C + √ C2 + 4a2 2 . The negative root is inadmissible. Since the material-region field increases continuously from zero to its boundary value, this positive root lies between a and b. Physical check The result tends to b/2 as a →0, agreeing with the uniform solid-cylinder interior field.

Question 3

A hollow insulating cylinder begins building field only beyond its inner radius

An infinite insulating tube occupies a<r<ba<r<b and carries uniform fixed density ρ>0\rho>0. Its hollow core and exterior contain no charge. There are no other sources.

Diagram shown in the original SVG worksheet.

  1. Derive the radial field in all three regions.

  2. Find the radius within the charged material where the field equals half its value at b. Define C=(b2−a2)/(2b)C=(b^2-a^2)/(2b) to simplify the algebra.

Question 3 - Solution

A hollow insulating cylinder begins building field only beyond its inner radius

Diagram shown in the original SVG worksheet.

(a) Method and calculation

λenc={0,r<a,πρ(r2−a2),a<r<b,πρ(b2−a2),r>b.\lambda_{\mathrm{enc}}=\begin{cases}0,&r<a,\\\pi\rho(r^2-a^2),&a<r<b,\\\pi\rho(b^2-a^2),&r>b.\end{cases}Er=λenc2πϵ0r.E_r=\frac{\lambda_{\mathrm{enc}}}{2\pi\epsilon_0r}.

(b) Interpretation and further calculation

ρ2ϵ0(r−a2r)=ρ(b2−a2)4ϵ0b⇒r2−Cr−a2=0.\frac\rho{2\epsilon_0}\left(r-\frac{a^2}r\right)=\frac{\rho(b^2-a^2)}{4\epsilon_0b}\Rightarrow r^2-Cr-a^2=0.r1/2=C+C2+4a22.r_{1/2}=\frac{C+\sqrt{C^2+4a^2}}2.The negative root is inadmissible. Since the material-region field increases continuously from zero to its boundary value, this positive root lies between a and b.

Physical check

The result tends to b/2b/2 as a→0a\to0, agreeing with the uniform solid-cylinder interior field.