Magnetic Force on a Current-Carrying Wire — Question 3

Section 28-7 · Physics pages 4596–4597

Question 3 Suspension angle measures a horizontal magnetic force on a current-carrying wire A wire of length L=.200 m and mass .0500 kg carries I=4.00 A along +z. A uniform field +.300ˆy T acts on it. Two identical light suspension strings tilt by angle theta from vertical. The return leads exert negligible force. Use g=9.81 m/s squared. FB mg θ Suspension geometry; the wire is represented schematically, with current perpendicular to the force plane. (a) Find the magnetic force magnitude and string angle. (b) Find the tension in each string and its change if the current is reversed.
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Question 3 - Solution Suspension angle measures a horizontal magnetic force on a current-carrying wire FB mg θ (a) Method and calculation⃗ FB = ILˆz × Bˆy = −ILBˆx, FB = .240 N. tan θ = FB/(mg) = .240/.4905 ⇒θ = tan−1(.240/.4905). (b) Interpretation and further calculation 2T cos θ = mg ⇒T = 1 2 √ (mg)2 + F 2 B = .273034 N. I →−I : θ →−θ, T unchanged. Physical check The sign of the horizontal displacement changes under current reversal, but the force magnitudes and tensions do not.

Question 3

Suspension angle measures a horizontal magnetic force on a current-carrying wire

A wire of length L=.200 m and mass .0500 kg carries I=4.00 A along +z. A uniform field +.300ŷ+.300\hat y T acts on it. Two identical light suspension strings tilt by angle theta from vertical. The return leads exert negligible force. Use g=9.81 m/s squared.

Diagram shown in the original SVG worksheet.

  1. Find the magnetic force magnitude and string angle.

  2. Find the tension in each string and its change if the current is reversed.

Question 3 - Solution

Suspension angle measures a horizontal magnetic force on a current-carrying wire

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F→B=ILẑ×Bŷ=−ILBx̂,FB=.240N.\vec F_B=IL\hat z\times B\hat y=-ILB\hat x,\quad F_B=.240\,\mathrm N.tan⁡θ=FB/(mg)=.240/.4905⇒θ=tan⁡−1(.240/.4905).\tan\theta=F_B/(mg)=.240/.4905\Rightarrow\theta=\tan^{-1}(.240/.4905).

(b) Interpretation and further calculation

2Tcos⁡θ=mg⇒T=12(mg)2+FB2=.273034N.2T\cos\theta=mg\Rightarrow T=\tfrac12\sqrt{(mg)^2+F_B^2}=.273034\,\mathrm N.I→−I:θ→−θ,T unchanged.I\to-I:\quad\theta\to-\theta,\quad T\text{ unchanged}.

Physical check

The sign of the horizontal displacement changes under current reversal, but the force magnitudes and tensions do not.