Magnetic Force on a Current-Carrying Wire — Question 10

Section 28-7 · Physics pages 4610–4611

Question 10 A moving current-carrying rod exchanges mechanical power with the maintained current source A rod of length L along +y carries maintained current I upward and moves with speed u along +x in a uniform field Bˆz. Use the supplied motional-emf relation Emot = ∫(⃗u ×⃗B) · d⃗ℓ, integrated upward along the rod. I u⃗ B = Bˆz Schematic; labels, not drawing lengths, specify the data. (a) Find the rod force and the mechanical power delivered by the magnetic interaction. (b) Find the signed motional emf and verify the relation between mechanical power and the electrical power needed to oppose this emf.
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Question 10 - Solution A moving current-carrying rod exchanges mechanical power with the maintained current source I u⃗ B = Bˆz (a) Method and calculation⃗ F = ILˆy × Bˆz = ILBˆx. Pmech =⃗F ·⃗u = ILBu. (b) Interpretation and further calculation⃗ u ×⃗B = −uBˆy ⇒Emot = −uBL. Pmech = −IEmot = IuBL. The maintained-current source supplies the converted energy, in addition to any resistive losses. Physical check There is no contradiction with zero magnetic work on an individual charge: the full circuit and source supply the mechanical energy.

Question 10

A moving current-carrying rod exchanges mechanical power with the maintained current source

A rod of length L along +y carries maintained current I upward and moves with speed u along +x in a uniform field BẑB\hat z. Use the supplied motional-emf relation ℰmot=∫(u→×B→)⋅dℓ→\mathcal E_{\mathrm{mot}}=\int(\vec u\times\vec B)\cdot d\vec\ell, integrated upward along the rod.

Diagram shown in the original SVG worksheet.

  1. Find the rod force and the mechanical power delivered by the magnetic interaction.

  2. Find the signed motional emf and verify the relation between mechanical power and the electrical power needed to oppose this emf.

Question 10 - Solution

A moving current-carrying rod exchanges mechanical power with the maintained current source

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F→=ILŷ×Bẑ=ILBx̂.\vec F=IL\hat y\times B\hat z=ILB\hat x.Pmech=F→⋅u→=ILBu.P_{\mathrm{mech}}=\vec F\cdot\vec u=ILBu.

(b) Interpretation and further calculation

u→×B→=−uBŷ⇒ℰmot=−uBL.\vec u\times\vec B=-uB\hat y\Rightarrow\mathcal E_{\mathrm{mot}}=-uBL.Pmech=−Iℰmot=IuBL.P_{\mathrm{mech}}=-I\mathcal E_{\mathrm{mot}}=IuBL.The maintained-current source supplies the converted energy, in addition to any resistive losses.

Physical check

There is no contradiction with zero magnetic work on an individual charge: the full circuit and source supply the mechanical energy.