Ampère's Law — Question 4

Section 29-3 · Physics pages 4698–4699

Question 4 A radial current-density profile changes the interior field without changing the exterior law An infinite cylindrical conductor of radius a has steady axial current density Jz(r) = J0r/a for r between zero and a, with J0 positive. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. r a current along +z Jz ∝r Schematic; labels, not drawing lengths, specify the data. (a) Find the total current and interior magnetic field. (b) Express B(r) in terms of the measured total current I and compare the interior field at r=a/2 with that of a uniform-current conductor having the same I and a.
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Question 4 - Solution A radial current-density profile changes the interior field without changing the exterior law r a current along +z Jz ∝r (a) Method and calculation Ienc(r) = ∫r 0 J0s a 2πs ds = 2πJ0r3 3a , I = 2πJ0a2 3 . B(r) = µ0Ienc 2πr = µ0J0r2 3a (r < a). (b) Interpretation and further calculation B(r) = µ0Ir2 2πa3 , B(a/2) = 1 4B(a). Buniform(a/2) = 1 2B(a) ⇒B/Buniform = 1/2 at r = a/2. Physical check Both distributions produce the same exterior field because they have the same total current and cylindrical symmetry.

Question 4

A radial current-density profile changes the interior field without changing the exterior law

An infinite cylindrical conductor of radius a has steady axial current density Jz(r)=J0r/aJ_z(r)=J_0r/a for r between zero and a, with J0 positive. 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 total current and interior magnetic field.

  2. Express B(r) in terms of the measured total current I and compare the interior field at r=a/2 with that of a uniform-current conductor having the same I and a.

Question 4 - Solution

A radial current-density profile changes the interior field without changing the exterior law

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ienc(r)=∫0rJ0sa2πsds=2πJ0r33a,I=2πJ0a23.I_{\mathrm{enc}}(r)=\int_0^r\frac{J_0s}{a}2\pi s\,ds=\frac{2\pi J_0r^3}{3a},\quad I=\frac{2\pi J_0a^2}{3}.B(r)=μ0Ienc2πr=μ0J0r23a(r<a).B(r)=\frac{\mu_0I_{\mathrm{enc}}}{2\pi r}=\boxed{\frac{\mu_0J_0r^2}{3a}}\quad(r<a).

(b) Interpretation and further calculation

B(r)=μ0Ir22πa3,B(a/2)=14B(a).B(r)=\frac{\mu_0Ir^2}{2\pi a^3},\quad B(a/2)=\frac14B(a).Buniform(a/2)=12B(a)⇒B/Buniform=1/2 at r=a/2.B_{\mathrm{uniform}}(a/2)=\frac12B(a)\Rightarrow\boxed{B/B_{\mathrm{uniform}}=1/2}\text{ at }r=a/2.

Physical check

Both distributions produce the same exterior field because they have the same total current and cylindrical symmetry.