Ohm's Law — Question 8

Section 26-4 · Physics pages 4226–4227

Question 8 An anisotropic ohmic medium can carry current away from the field direction A planar medium obeys Jx = 2σEx and Jy = σEy. The imposed field is⃗E = E0(ˆx + ˆy)/ √ 2, with positive sigma and E0. Ignore boundaries. x y⃗ E⃗ J Schematic; labels, not drawing lengths, specify the data. (a) Find current magnitude and its angle to x. (b) Find the component of J perpendicular to E, using ˆt = (−ˆx + ˆy)/ √ 2, and assess whether response is linear.
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Question 8 - Solution An anisotropic ohmic medium can carry current away from the field direction x y⃗ E⃗ J (a) Method and calculation⃗ J = σE0 √ 2 (2ˆx + ˆy), |⃗J| = σE0 √ 5/2. θJ = tan−1(1/2) = 26.565◦. (b) Interpretation and further calculation J⊥=⃗J · ˆt = −σE0/2.⃗ J(a⃗E1 + b⃗E2) = a⃗J(⃗E1) + b⃗J(⃗E2). A constant conductivity tensor is linear even when J and E are not parallel. Physical check Scalar resistivity presumes isotropy; linearity itself is a broader property.

Question 8

An anisotropic ohmic medium can carry current away from the field direction

A planar medium obeys Jx=2σExJ_x=2\sigma E_x and Jy=σEyJ_y=\sigma E_y. The imposed field is E→=E0(x̂+ŷ)/2\vec E=E_0(\hat x+\hat y)/\sqrt2, with positive sigma and E0. Ignore boundaries.

Diagram shown in the original SVG worksheet.

  1. Find current magnitude and its angle to x.

  2. Find the component of J perpendicular to E, using t̂=(−x̂+ŷ)/2\hat t=(-\hat x+\hat y)/\sqrt2, and assess whether response is linear.

Question 8 - Solution

An anisotropic ohmic medium can carry current away from the field direction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

J→=σE02(2x̂+ŷ),|J→|=σE05/2.\vec J=\frac{\sigma E_0}{\sqrt2}(2\hat x+\hat y),\quad |\vec J|=\sigma E_0\sqrt{5/2}.θJ=tan⁡−1(1/2)=26.565∘.\theta_J=\tan^{-1}(1/2)=26.565^\circ.

(b) Interpretation and further calculation

J⟂=J→⋅t̂=−σE0/2.J_\perp=\vec J\cdot\hat t=-\sigma E_0/2.J→(aE→1+bE→2)=aJ→(E→1)+bJ→(E→2).\vec J(a\vec E_1+b\vec E_2)=a\vec J(\vec E_1)+b\vec J(\vec E_2).A constant conductivity tensor is linear even when J and E are not parallel.

Physical check

Scalar resistivity presumes isotropy; linearity itself is a broader property.