The Definition of B — Question 4

Section 28-2 · Physics pages 4498–4499

Question 4 Two perpendicular velocity probes determine all three magnetic-field components A positive test charge q=1.00 microcoulomb is sent through the same field with velocity 104ˆx m/s, giving force (0, −.0300, .0200) N. With velocity 104ˆy m/s, its force is (.0300, 0, −.0100) N. Only magnetic forces are present. x y⃗ v1⃗ v2 same unknown⃗B Schematic; labels, not drawing lengths, specify the data. (a) Reconstruct B from both measurements. (b) Predict the force for velocity 104ˆz m/s and verify it is perpendicular to that velocity.
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Question 4 - Solution Two perpendicular velocity probes determine all three magnetic-field components x y⃗ v1⃗ v2 same unknown⃗B (a) Method and calculation⃗ Fx = qu(0, −Bz, By),⃗ Fy = qu(Bz, 0, −Bx), qu = .0100.⃗ B = (1.00ˆx + 2.00ˆy + 3.00ˆz) T. (b) Interpretation and further calculation⃗ Fz = qu(−By, Bx, 0) = (−.0200ˆx + .0100ˆy) N.⃗ Fz · (uˆz) = 0. Physical check A field component invisible to one velocity direction is accessible to a nonparallel probe.

Question 4

Two perpendicular velocity probes determine all three magnetic-field components

A positive test charge q=1.00 microcoulomb is sent through the same field with velocity 104x̂10^4\hat x m/s, giving force (0,−.0300,.0200)(0,-.0300,.0200) N. With velocity 104ŷ10^4\hat y m/s, its force is (.0300,0,−.0100)(.0300,0,-.0100) N. Only magnetic forces are present.

Diagram shown in the original SVG worksheet.

  1. Reconstruct B from both measurements.

  2. Predict the force for velocity 104ẑ10^4\hat z m/s and verify it is perpendicular to that velocity.

Question 4 - Solution

Two perpendicular velocity probes determine all three magnetic-field components

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F→x=qu(0,−Bz,By),F→y=qu(Bz,0,−Bx),qu=.0100.\vec F_x=qu(0,-B_z,B_y),\quad\vec F_y=qu(B_z,0,-B_x),\quad qu=.0100.B→=(1.00x̂+2.00ŷ+3.00ẑ)T.\vec B=(1.00\hat x+2.00\hat y+3.00\hat z)\,\mathrm T.

(b) Interpretation and further calculation

F→z=qu(−By,Bx,0)=(−.0200x̂+.0100ŷ)N.\vec F_z=qu(-B_y,B_x,0)=(-.0200\hat x+.0100\hat y)\,\mathrm N.F→z⋅(uẑ)=0.\vec F_z\cdot(u\hat z)=0.

Physical check

A field component invisible to one velocity direction is accessible to a nonparallel probe.