Induced Electric Fields — Question 7

Section 30-5 · Physics pages 4844–4845

Question 7 An added electrostatic field can cancel induction locally without changing its circulation Inside a cylinder, a uniform axial field increases at rate beta. Its induced electric field is⃗ Eind = (β/2)(yˆx −xˆy). Add a uniform electrostatic field E0ˆx, with E0 and beta positive. x y null E0ˆx Schematic; labels, not drawing lengths, specify the data. (a) Find the point where the total electric field vanishes, assuming it lies inside the cylinder of radius a. (b) Find the circulation around a concentric circle of radius r<a and the condition for that zero-field point to lie inside.
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Question 7 - Solution An added electrostatic field can cancel induction locally without changing its circulation x y null E0ˆx (a) Method and calculation Ex = E0 + βy/2 = 0, Ey = −βx/2 = 0. (x, y) = (0, −2E0/β) . (b) Interpretation and further calculation I⃗ E · d⃗ℓ= I⃗ Eind · d⃗ℓ+ E0 I dx = −πr2β . 2E0/β < a . Physical check Zero total field at one point does not remove a nonzero circulation around a larger contour.

Question 7

An added electrostatic field can cancel induction locally without changing its circulation

Inside a cylinder, a uniform axial field increases at rate beta. Its induced electric field is E→ind=(β/2)(yx̂−xŷ)\vec E_{\mathrm{ind}}=(\beta/2)(y\hat x-x\hat y). Add a uniform electrostatic field E0x̂E_0\hat x, with E0 and beta positive.

Diagram shown in the original SVG worksheet.

  1. Find the point where the total electric field vanishes, assuming it lies inside the cylinder of radius a.

  2. Find the circulation around a concentric circle of radius r<a and the condition for that zero-field point to lie inside.

Question 7 - Solution

An added electrostatic field can cancel induction locally without changing its circulation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=E0+βy/2=0,Ey=−βx/2=0.E_x=E_0+\beta y/2=0,\quad E_y=-\beta x/2=0.(x,y)=(0,−2E0/β).\boxed{(x,y)=(0,-2E_0/\beta)}.

(b) Interpretation and further calculation

∮E→⋅dℓ→=∮E→ind⋅dℓ→+E0∮dx=−πr2β.\oint\vec E\cdot d\vec\ell=\oint\vec E_{\mathrm{ind}}\cdot d\vec\ell+E_0\oint dx=\boxed{-\pi r^2\beta}.2E0/β<a.\boxed{2E_0/\beta<a}.

Physical check

Zero total field at one point does not remove a nonzero circulation around a larger contour.