Ampère's Law — Question 10

Section 29-3 · Physics pages 4710–4711

Question 10 A cylindrical surface current produces a field jump that a volume current cannot A long cylinder of radius a carries uniform axial volume current density J inside and an additional infinitesimally thin axial surface current Kˆz on its boundary. K may be negative. There are no other currents. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. r a current along +z surface Kˆz Schematic; labels, not drawing lengths, specify the data. (a) Find the fields immediately inside and outside the boundary and their difference. (b) Choose K so the exterior field vanishes everywhere. Find the remaining interior field.
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Question 10 - Solution A cylindrical surface current produces a field jump that a volume current cannot r a current along +z surface Kˆz (a) Method and calculation Bϕ(a−) = µ0Ja 2 , Itotal = Jπa2 + K(2πa). Bϕ(a+) = µ0(Ja/2 + K), Bϕ(a+) −Bϕ(a−) = µ0K . (b) Interpretation and further calculation Itotal = 0 ⇒K = −Ja/2 . Bϕ(r) = µ0Jr/2 (r < a), Bϕ(r) = 0 (r > a) . Physical check A surface-current sheet can sustain a discontinuity of tangential magnetic field; zero exterior field does not imply zero interior field.

Question 10

A cylindrical surface current produces a field jump that a volume current cannot

A long cylinder of radius a carries uniform axial volume current density J inside and an additional infinitesimally thin axial surface current KẑK\hat z on its boundary. K may be negative. There are no other currents. Use vacuum permeability μ0≃4π×10−7Tm/A\mu_0\simeq4\pi\times10^{-7}\,\mathrm{T\,m/A} where numerical values are needed.

Diagram shown in the original SVG worksheet.

  1. Find the fields immediately inside and outside the boundary and their difference.

  2. Choose K so the exterior field vanishes everywhere. Find the remaining interior field.

Question 10 - Solution

A cylindrical surface current produces a field jump that a volume current cannot

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Bϕ(a−)=μ0Ja2,Itotal=Jπa2+K(2πa).B_\phi(a^-)=\frac{\mu_0Ja}{2},\quad I_{\mathrm{total}}=J\pi a^2+K(2\pi a).Bϕ(a+)=μ0(Ja/2+K),Bϕ(a+)−Bϕ(a−)=μ0K.B_\phi(a^+)=\mu_0(Ja/2+K),\quad\boxed{B_\phi(a^+)-B_\phi(a^-)=\mu_0K}.

(b) Interpretation and further calculation

Itotal=0⇒K=−Ja/2.I_{\mathrm{total}}=0\Rightarrow\boxed{K=-Ja/2}.Bϕ(r)=μ0Jr/2(r<a),Bϕ(r)=0(r>a).\boxed{B_\phi(r)=\mu_0Jr/2\ (r<a),\qquad B_\phi(r)=0\ (r>a)}.

Physical check

A surface-current sheet can sustain a discontinuity of tangential magnetic field; zero exterior field does not imply zero interior field.