Flux of an Electric Field — Question 3

Section 23-2 · Physics pages 3656–3657

Question 3 A transverse uniform field crosses a cylinder without net side flux A closed cylinder has radius R, length L and axis z. A uniform electric field is E = E⊥ˆx + E∥ˆz. Orient every surface outward. axis z Closed finite cylinder; both end faces belong to the surface. (a) Find the flux through each end and through the curved side. (b) For E⊥> 0, integrate the positive outward flux over the half of the curved side where cos ϕ > 0. Compare it with the net side flux.
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Question 3 - Solution A transverse uniform field crosses a cylinder without net side flux axis z (a) Method and calculation Φtop = E∥πR2, Φbottom = −E∥πR2. Φside = E⊥RL ∫2π 0 cos ϕ dϕ = 0. (b) Interpretation and further calculation Φside,+ = E⊥RL ∫π/2 −π/2 cos ϕ dϕ = 2E⊥RL. Φside,−= −2E⊥RL, Φclosed = 0. A zero side integral arises from cancellation, not from a field tangent everywhere. Physical check The transverse field is normal to the cylinder at some points and tangent at others.

Question 3

A transverse uniform field crosses a cylinder without net side flux

A closed cylinder has radius R, length L and axis z. A uniform electric field is 𝑬=E⟂𝒙̂+E∥𝒛̂\mathbf E=E_\perp\hat{\mathbf x}+E_\parallel\hat{\mathbf z}. Orient every surface outward.

Diagram shown in the original SVG worksheet.

  1. Find the flux through each end and through the curved side.

  2. For E⟂>0E_\perp>0, integrate the positive outward flux over the half of the curved side where cos⁡ϕ>0\cos\phi>0. Compare it with the net side flux.

Question 3 - Solution

A transverse uniform field crosses a cylinder without net side flux

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φtop=E∥πR2,Φbottom=−E∥πR2.\Phi_{\mathrm{top}}=E_\parallel\pi R^2,\quad\Phi_{\mathrm{bottom}}=-E_\parallel\pi R^2.Φside=E⟂RL∫02πcos⁡ϕdϕ=0.\Phi_{\mathrm{side}}=E_\perp RL\int_0^{2\pi}\cos\phi\,d\phi=0.

(b) Interpretation and further calculation

Φside,+=E⟂RL∫−π/2π/2cos⁡ϕdϕ=2E⟂RL.\Phi_{\mathrm{side,+}}=E_\perp RL\int_{-\pi/2}^{\pi/2}\cos\phi\,d\phi=2E_\perp RL.Φside,−=−2E⟂RL,Φclosed=0.\Phi_{\mathrm{side,-}}=-2E_\perp RL,\quad\Phi_{\mathrm{closed}}=0.A zero side integral arises from cancellation, not from a field tangent everywhere.

Physical check

The transverse field is normal to the cylinder at some points and tangent at others.