Magnetic Force on a Current-Carrying Wire — Question 7

Section 28-7 · Physics pages 4604–4605

Question 7 A closed rectangular loop acquires net force in a spatially varying field A rectangular loop spans 0<x<a and 0<y<b and carries counterclockwise current I viewed from +z. The external field is⃗B(x) = (B0 + gx)ˆz. Assume the entire loop lies where this prescribed field model holds. I b a Bz increases Schematic; labels, not drawing lengths, specify the data. (a) Find the forces on the two vertical sides and show how the horizontal-side forces combine. (b) Find the total force and its direction for g positive; explain why the uniform-field cancellation no longer applies.
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Question 7 - Solution A closed rectangular loop acquires net force in a spatially varying field I b a Bz increases (a) Method and calculation⃗ Fright = Ib(B0 + ga)ˆx,⃗ Fleft = −IbB0ˆx.⃗ Fbottom = −I ∫a 0 (B0 + gx)dx ˆy = −⃗Ftop. (b) Interpretation and further calculation⃗ Ftotal = Iabgˆx. g > 0 ⇒⃗Ftotal points toward increasing Bz. Physical check Opposite sides sample different magnetic fields, so their equal currents do not imply equal opposing forces.

Question 7

A closed rectangular loop acquires net force in a spatially varying field

A rectangular loop spans 0<x<a and 0<y<b and carries counterclockwise current I viewed from +z. The external field is B→(x)=(B0+gx)ẑ\vec B(x)=(B_0+gx)\hat z. Assume the entire loop lies where this prescribed field model holds.

Diagram shown in the original SVG worksheet.

  1. Find the forces on the two vertical sides and show how the horizontal-side forces combine.

  2. Find the total force and its direction for g positive; explain why the uniform-field cancellation no longer applies.

Question 7 - Solution

A closed rectangular loop acquires net force in a spatially varying field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F→right=Ib(B0+ga)x̂,F→left=−IbB0x̂.\vec F_{\mathrm{right}}=Ib(B_0+ga)\hat x,\quad\vec F_{\mathrm{left}}=-IbB_0\hat x.F→bottom=−I∫0a(B0+gx)dxŷ=−F→top.\vec F_{\mathrm{bottom}}=-I\int_0^a(B_0+gx)dx\,\hat y=-\vec F_{\mathrm{top}}.

(b) Interpretation and further calculation

F→total=Iabgx̂.\vec F_{\mathrm{total}}=Iabg\hat x.g>0⇒F→total points toward increasing Bz.g>0\Rightarrow\vec F_{\mathrm{total}}\text{ points toward increasing }B_z.

Physical check

Opposite sides sample different magnetic fields, so their equal currents do not imply equal opposing forces.