Force Between Two Parallel Currents — Question 6

Section 29-2 · Physics pages 4682–4683

Question 6 A rectangular loop near a straight wire experiences an unbalanced pair of parallel forces A long wire lies on the y axis carrying I upward. A rectangular loop in the xy plane spans x=a to x=a+w and has height ell. Its current i runs upward on the near side x=a and downward on the far side. Ignore the loop self-field. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I i a w ℓ Schematic; labels, not drawing lengths, specify the data. (a) Find the net force on the loop due to the long wire. (b) For w much smaller than a, derive the leading force and explain the cancellation of the top and bottom forces.
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Question 6 - Solution A rectangular loop near a straight wire experiences an unbalanced pair of parallel forces I i a w ℓ (a) Method and calculation⃗ fnear = −µ0Iiℓ 2πa ˆx,⃗ ffar = + µ0Iiℓ 2π(a + w) ˆx.⃗ F = −µ0Iiℓ 2π (1 a − 1 a + w ) ˆx . (b) Interpretation and further calculation 1 a − 1 a + w = w a(a + w) ≃w a2 ⇒⃗F ≃−µ0Iiℓw 2πa2 ˆx.⃗ Ftop +⃗Fbottom = 0 because their equal field profiles meet opposite d⃗ℓ. Physical check The near attractive side wins over the far repulsive side because the long-wire field decreases with distance.

Question 6

A rectangular loop near a straight wire experiences an unbalanced pair of parallel forces

A long wire lies on the y axis carrying I upward. A rectangular loop in the xy plane spans x=a to x=a+w and has height ell. Its current i runs upward on the near side x=a and downward on the far side. Ignore the loop self-field. 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 net force on the loop due to the long wire.

  2. For w much smaller than a, derive the leading force and explain the cancellation of the top and bottom forces.

Question 6 - Solution

A rectangular loop near a straight wire experiences an unbalanced pair of parallel forces

Diagram shown in the original SVG worksheet.

(a) Method and calculation

f→near=−μ0Iiℓ2πax̂,f→far=+μ0Iiℓ2π(a+w)x̂.\vec f_{\mathrm{near}}=-\frac{\mu_0Ii\ell}{2\pi a}\hat x,\quad\vec f_{\mathrm{far}}=+\frac{\mu_0Ii\ell}{2\pi(a+w)}\hat x.F→=−μ0Iiℓ2π(1a−1a+w)x̂.\boxed{\vec F=-\frac{\mu_0Ii\ell}{2\pi}\left(\frac1a-\frac1{a+w}\right)\hat x}.

(b) Interpretation and further calculation

1a−1a+w=wa(a+w)≃wa2⇒F→≃−μ0Iiℓw2πa2x̂.\frac1a-\frac1{a+w}=\frac{w}{a(a+w)}\simeq\frac w{a^2}\Rightarrow\vec F\simeq-\frac{\mu_0Ii\ell w}{2\pi a^2}\hat x.F→top+F→bottom=0because their equal field profiles meet opposite dℓ→.\vec F_{\mathrm{top}}+\vec F_{\mathrm{bottom}}=0\quad\text{because their equal field profiles meet opposite }d\vec\ell.

Physical check

The near attractive side wins over the far repulsive side because the long-wire field decreases with distance.