Maxwell's Equations — Question 6

Section 32-4 · Physics pages 5242–5243

Question 6 A prescribed nonuniform magnetic ramp determines an electric curl and a current In a region let Bz = βxt, Bx = By = 0, and seek E = Ey(x)ˆy with Ey(0) = 0. Use vacuum Maxwell equations. x Ey Schematic; labels, not drawing lengths, specify the data. (a) Find Ey from Faraday law. (b) Find rho and J needed for this field pair.
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Question 6 - Solution A prescribed nonuniform magnetic ramp determines an electric curl and a current x Ey (a) Method and calculation ∂xEy = −∂tBz = −βx ⇒Ey = −βx2/2 . ∇· E = ∂yEy = 0 ⇒ρ = 0 . (b) Interpretation and further calculation (∇× B)y = −∂xBz = −βt, ∂tE = 0. J = −(βt/µ0)ˆy, ∇· J = 0 . Physical check A changing B need not require a changing E; a static electric curl can accompany a constant magnetic ramp rate.

Question 6

A prescribed nonuniform magnetic ramp determines an electric curl and a current

In a region let Bz=βxtB_z=\beta xt, Bx=By=0B_x=B_y=0, and seek 𝑬=Ey(x)ŷ\mathbf E=E_y(x)\hat y with Ey(0)=0E_y(0)=0. Use vacuum Maxwell equations.

Diagram shown in the original SVG worksheet.

  1. Find Ey from Faraday law.

  2. Find rho and J needed for this field pair.

Question 6 - Solution

A prescribed nonuniform magnetic ramp determines an electric curl and a current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂xEy=−∂tBz=−βx⇒Ey=−βx2/2.\partial_xE_y=-\partial_tB_z=-\beta x\Rightarrow\boxed{E_y=-\beta x^2/2}.∇⋅𝑬=∂yEy=0⇒ρ=0.\nabla\cdot\mathbf E=\partial_yE_y=0\Rightarrow\boxed{\rho=0}.

(b) Interpretation and further calculation

(∇×𝑩)y=−∂xBz=−βt,∂t𝑬=0.(\nabla\times\mathbf B)_y=-\partial_xB_z=-\beta t,\quad\partial_t\mathbf E=0.𝑱=−(βt/μ0)ŷ,∇⋅𝑱=0.\boxed{\mathbf J=-(\beta t/\mu_0)\hat y,\quad\nabla\cdot\mathbf J=0}.

Physical check

A changing B need not require a changing E; a static electric curl can accompany a constant magnetic ramp rate.