Ampère's Law — Question 9

Section 29-3 · Physics pages 4708–4709

Question 9 A measured azimuthal field reconstructs the enclosed current and its density Inside an axially symmetric long conductor, measurements give Bϕ(r) = kr2 for 0 ≤r ≤a, with k positive. The field outside comes only from this conductor. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. r a current along +z measured Bϕ = kr2 Schematic; labels, not drawing lengths, specify the data. (a) Infer the axial current density as a function of r and the total current. (b) For k=.500 T/m squared and a=.0200 m, find I and the exterior field at r=.0600 m.
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Question 9 - Solution A measured azimuthal field reconstructs the enclosed current and its density r a current along +z measured Bϕ = kr2 (a) Method and calculation Ienc(r) = 2πrBϕ µ0 = 2πkr3 µ0 , dI = Jz(r)2πr dr. Jz(r) = 3kr µ0 , I = 2πka3 µ0 . (b) Interpretation and further calculation I = 2π(.500)(.0200)3 4π × 10−7 = 20.0 A . B(.0600) = µ0(20.0) 2π(.0600) = 66.6667 µT . Physical check Differentiating enclosed current, rather than simply dividing total current by area, recovers the nonuniform density.

Question 9

A measured azimuthal field reconstructs the enclosed current and its density

Inside an axially symmetric long conductor, measurements give Bϕ(r)=kr2B_\phi(r)=kr^2 for 0≤r≤a0\le r\le a, with k positive. The field outside comes only from this conductor. 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. Infer the axial current density as a function of r and the total current.

  2. For k=.500 T/m squared and a=.0200 m, find I and the exterior field at r=.0600 m.

Question 9 - Solution

A measured azimuthal field reconstructs the enclosed current and its density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ienc(r)=2πrBϕμ0=2πkr3μ0,dI=Jz(r)2πrdr.I_{\mathrm{enc}}(r)=\frac{2\pi rB_\phi}{\mu_0}=\frac{2\pi kr^3}{\mu_0},\quad dI=J_z(r)2\pi r\,dr.Jz(r)=3krμ0,I=2πka3μ0.\boxed{J_z(r)=\frac{3kr}{\mu_0},\quad I=\frac{2\pi ka^3}{\mu_0}}.

(b) Interpretation and further calculation

I=2π(.500)(.0200)34π×10−7=20.0A.I=\frac{2\pi(.500)(.0200)^3}{4\pi\times10^{-7}}=\boxed{20.0\,\mathrm A}.B(.0600)=μ0(20.0)2π(.0600)=66.6667μT.B(.0600)=\frac{\mu_0(20.0)}{2\pi(.0600)}=\boxed{66.6667\,\mu\mathrm T}.

Physical check

Differentiating enclosed current, rather than simply dividing total current by area, recovers the nonuniform density.