Current Density — Question 6

Section 26-2 · Physics pages 4182–4183

Question 6 A spatially increasing current density depletes local charge Within a slab 0 < x < L,⃗J = (J0 + ax)ˆx, where a is constant in time and has units A/m3. Initially ρq = ρ0. There is no lateral flux. A +x J0 J0 + aL Wire cross-section and reference direction; dimensions are schematic. (a) Use ∂ρq/∂t + ∇·⃗J = 0 to find the charge density. (b) For slab area A, verify the total charge change directly from endpoint currents.
Show solutionHide solution
Question 6 - Solution A spatially increasing current density depletes local charge A +x J0 J0 + aL (a) Method and calculation ∇·⃗J = ∂Jx/∂x = a. ρq(x, t) = ρ0 −at. (b) Interpretation and further calculation Iin = AJ0, Iout = A(J0 + aL). dQ/dt = Iin −Iout = −aAL = AL ∂ρq/∂t. Physical check Positive divergence removes positive charge from a volume; it does not create charge.

Question 6

A spatially increasing current density depletes local charge

Within a slab 0<x<L0<x<L, J→=(J0+ax)x̂\vec J=(J_0+ax)\hat x, where a is constant in time and has units A/m3^3. Initially ρq=ρ0\rho_q=\rho_0. There is no lateral flux.

Diagram shown in the original SVG worksheet.

  1. Use ∂ρq/∂t+∇⋅J→=0\partial\rho_q/\partial t+\nabla\cdot\vec J=0 to find the charge density.

  2. For slab area A, verify the total charge change directly from endpoint currents.

Question 6 - Solution

A spatially increasing current density depletes local charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∇⋅J→=∂Jx/∂x=a.\nabla\cdot\vec J=\partial J_x/\partial x=a.ρq(x,t)=ρ0−at.\rho_q(x,t)=\rho_0-at.

(b) Interpretation and further calculation

Iin=AJ0,Iout=A(J0+aL).I_{\mathrm{in}}=AJ_0,\quad I_{\mathrm{out}}=A(J_0+aL).dQ/dt=Iin−Iout=−aAL=AL∂ρq/∂t.dQ/dt=I_{\mathrm{in}}-I_{\mathrm{out}}=-aAL=AL\,\partial\rho_q/\partial t.

Physical check

Positive divergence removes positive charge from a volume; it does not create charge.