Calculating the Magnetic Field Due to a Current — Question 1

Section 29-1 · Physics pages 4652–4653

Question 1 A finite straight segment approaches the long-wire field in a controlled limit A straight segment on the x axis extends from −L to +L and carries steady current I toward +x. Find only this segment contribution at P = (0, a, 0); the rest of the closed circuit is distant. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I P a −L +L Schematic; labels, not drawing lengths, specify the data. (a) Integrate the Biot–Savart law to obtain the field vector. (b) Evaluate for I=3.00 A, L=.120 m and a=.0500 m, and compare with an infinite wire.
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Question 1 - Solution A finite straight segment approaches the long-wire field in a controlled limit I P a −L +L (a) Method and calculation d⃗ℓ= dxˆx,⃗ r = −xˆx + aˆy, d⃗ℓ×⃗r = a dxˆz.⃗ B = µ0I 4π ∫L −L a dx (x2 + a2)3/2 ˆz = µ0IL 2πa √ L2 + a2 ˆz . (b) Interpretation and further calculation B = (12.0 µT).120 .130 = 11.0769 µT . B∞= µ0I 2πa = 12.0 µT, B/B∞= 12/13. Physical check The field points out of the xy plane. The finite segment contributes less than the infinite wire, with equality approached as L/a grows.

Question 1

A finite straight segment approaches the long-wire field in a controlled limit

A straight segment on the x axis extends from −L-L to +L+L and carries steady current I toward +x. Find only this segment contribution at P=(0,a,0)P=(0,a,0); the rest of the closed circuit is distant. 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. Integrate the Biot–Savart law to obtain the field vector.

  2. Evaluate for I=3.00 A, L=.120 m and a=.0500 m, and compare with an infinite wire.

Question 1 - Solution

A finite straight segment approaches the long-wire field in a controlled limit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dℓ→=dxx̂,r→=−xx̂+aŷ,dℓ→×r→=adxẑ.d\vec\ell=dx\hat x,\quad\vec r=-x\hat x+a\hat y,\quad d\vec\ell\times\vec r=a\,dx\hat z.B→=μ0I4π∫−LLadx(x2+a2)3/2ẑ=μ0IL2πaL2+a2ẑ.\vec B=\frac{\mu_0 I}{4\pi}\int_{-L}^L\frac{a\,dx}{(x^2+a^2)^{3/2}}\hat z=\boxed{\frac{\mu_0 I L}{2\pi a\sqrt{L^2+a^2}}\hat z}.

(b) Interpretation and further calculation

B=(12.0μT).120.130=11.0769μT.B=(12.0\,\mu\mathrm T)\frac{.120}{.130}=\boxed{11.0769\,\mu\mathrm T}.B∞=μ0I2πa=12.0μT,B/B∞=12/13.B_\infty=\frac{\mu_0 I}{2\pi a}=12.0\,\mu\mathrm T,\quad B/B_\infty=12/13.

Physical check

The field points out of the xy plane. The finite segment contributes less than the infinite wire, with equality approached as L/a grows.