Magnetic Force on a Current-Carrying Wire — Question 1

Section 28-7 · Physics pages 4592–4593

Question 1 The directed length vector determines the force on a straight current segment A straight segment carries I=3.00 A from its first endpoint to its second, with directed displacement⃗L = (.200ˆx + .100ˆy) m. The uniform field is⃗B = (.400ˆx −.300ˆz) T. x y I,⃗L⃗ B = Bxˆx + Bzˆz Schematic; labels, not drawing lengths, specify the data. (a) Find the force vector and magnitude. (b) Verify that the force is perpendicular to both the segment and the magnetic field.
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Question 1 - Solution The directed length vector determines the force on a straight current segment x y I,⃗L⃗ B = Bxˆx + Bzˆz (a) Method and calculation⃗ L ×⃗B = (−.0300ˆx + .0600ˆy −.0400ˆz) T m.⃗ F = I⃗L ×⃗B = (−.0900ˆx + .180ˆy −.120ˆz) N, F = √ .0549 N. (b) Interpretation and further calculation⃗ F ·⃗L = (−.0900)(.200) + (.180)(.100) = 0.⃗ F ·⃗B = (−.0900)(.400) + (−.120)(−.300) = 0. Physical check The length vector follows conventional current, regardless of which microscopic charge carriers carry it.

Question 1

The directed length vector determines the force on a straight current segment

A straight segment carries I=3.00 A from its first endpoint to its second, with directed displacement L→=(.200x̂+.100ŷ)\vec L=(.200\hat x+.100\hat y) m. The uniform field is B→=(.400x̂−.300ẑ)\vec B=(.400\hat x-.300\hat z) T.

Diagram shown in the original SVG worksheet.

  1. Find the force vector and magnitude.

  2. Verify that the force is perpendicular to both the segment and the magnetic field.

Question 1 - Solution

The directed length vector determines the force on a straight current segment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

L→×B→=(−.0300x̂+.0600ŷ−.0400ẑ)Tm.\vec L\times\vec B=(-.0300\hat x+.0600\hat y-.0400\hat z)\,\mathrm{T\,m}.F→=IL→×B→=(−.0900x̂+.180ŷ−.120ẑ)N,F=.0549N.\vec F=I\vec L\times\vec B=(-.0900\hat x+.180\hat y-.120\hat z)\,\mathrm N,\quad F=\sqrt{.0549}\,\mathrm N.

(b) Interpretation and further calculation

F→⋅L→=(−.0900)(.200)+(.180)(.100)=0.\vec F\cdot\vec L=(-.0900)(.200)+(.180)(.100)=0.F→⋅B→=(−.0900)(.400)+(−.120)(−.300)=0.\vec F\cdot\vec B=(-.0900)(.400)+(-.120)(-.300)=0.

Physical check

The length vector follows conventional current, regardless of which microscopic charge carriers carry it.