Calculating the Magnetic Field Due to a Current — Question 8

Section 29-1 · Physics pages 4666–4667

Question 8 A semicircular detour and tangent leads reinforce at their common center A wire travels from x=-infinity to x=0 along y=-R, then counterclockwise around the right semicircle centered at the origin to (0,+R), then toward x=-infinity along y=+R. Current I follows this path. Find the field at the origin. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I P R Schematic; labels, not drawing lengths, specify the data. (a) Calculate the contributions of the semicircle and the two semi-infinite straight leads. (b) Find the total and the fraction supplied by the curved part.
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Question 8 - Solution A semicircular detour and tangent leads reinforce at their common center I P R (a) Method and calculation Barc = µ0Iπ 4πR = µ0I 4R , Blead = µ0I 4πR.⃗ Barc,⃗Blower,⃗Bupper all point along + z. (b) Interpretation and further calculation⃗ B = µ0I 4πR(π + 2)ˆz . Barc Btotal = π π + 2 = .611015. Physical check Tangent leads have a finite perpendicular distance from P; unlike radial leads, their fields do not vanish.

Question 8

A semicircular detour and tangent leads reinforce at their common center

A wire travels from x=-infinity to x=0 along y=-R, then counterclockwise around the right semicircle centered at the origin to (0,+R), then toward x=-infinity along y=+R. Current I follows this path. Find the field at the origin. 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. Calculate the contributions of the semicircle and the two semi-infinite straight leads.

  2. Find the total and the fraction supplied by the curved part.

Question 8 - Solution

A semicircular detour and tangent leads reinforce at their common center

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Barc=μ0Iπ4πR=μ0I4R,Blead=μ0I4πR.B_{\mathrm{arc}}=\frac{\mu_0 I\pi}{4\pi R}=\frac{\mu_0 I}{4R},\quad B_{\mathrm{lead}}=\frac{\mu_0 I}{4\pi R}.B→arc,B→lower,B→upper all point along +z.\vec B_{\mathrm{arc}},\ \vec B_{\mathrm{lower}},\ \vec B_{\mathrm{upper}}\text{ all point along }+z.

(b) Interpretation and further calculation

B→=μ0I4πR(π+2)ẑ.\vec B=\boxed{\frac{\mu_0 I}{4\pi R}(\pi+2)\hat z}.BarcBtotal=ππ+2=.611015.\frac{B_{\mathrm{arc}}}{B_{\mathrm{total}}}=\boxed{\frac{\pi}{\pi+2}}=.611015.

Physical check

Tangent leads have a finite perpendicular distance from P; unlike radial leads, their fields do not vanish.