Distinguish one segment force from whole-loop torque
A current-carrying segment in a uniform magnetic field experiences F=I L_vector cross B, where L_vector follows conventional current. Here the segment lies in the xy plane, has length .2 m and makes angle θ from +x toward +y. The magnetic field is .05 T along +x. Only the y component of the segment contributes, giving Fz=−I(.2)(.05)sinθ.
Learning outcome: Compare 0,30,90,180 degrees at fixed current. Retain signed z force rather than only magnitude. Sketch a rectangular closed loop and identify two forces that cancel as vectors but can still produce a torque.
Starting recap
Use a right-handed coordinate system, oriented surface normal, signed charge/current and declared energy boundary. Separate an entry force from a trajectory, emf from current, and rms from signed average.
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At θ=90 degrees and I=4 A, Fz=−4(.2)(.05)=−.04 N. At θ=30 degrees the same current gives −.02 N. At 0 or180 degrees it is exactly zero despite nonzero current and field.
Open the experimentPredict
A closed current loop in a spatially uniform magnetic field can have:
Experiment
Compare 0,30,90,180 degrees at fixed current. Retain signed z force rather than only magnitude. Sketch a rectangular closed loop and identify two forces that cancel as vectors but can still produce a torque.
Resolve the force on one current-carrying segment
Worked teaching model · synthetic values · Straight segment length .2 m in xy plane; uniform B=.05 T along +x. Current follows the segment orientation. Only this segment force is calculated; a closed loop in uniform field has separate forces whose vector sum is zero.
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One segment force versus orientation
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: I L cross B (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for One segment force versus orientation
I L cross B
| segment angle (degrees) | signed z force (N) |
|---|---|
| 0 | 0 |
| 4.5 | -0.00313836 |
| 9 | -0.00625738 |
| 13.5 | -0.00933781 |
| 18 | -0.0123607 |
| 22.5 | -0.0153073 |
| 27 | -0.0181596 |
| 31.5 | -0.0208999 |
| 36 | -0.0235114 |
| 40.5 | -0.0259779 |
| 45 | -0.0282843 |
| 49.5 | -0.0304162 |
| 54 | -0.0323607 |
| 58.5 | -0.0341056 |
| 63 | -0.0356403 |
| 67.5 | -0.0369552 |
| 72 | -0.0380423 |
| 76.5 | -0.0388948 |
| 81 | -0.0395075 |
| 85.5 | -0.0398767 |
| 90 | -0.04 |
| 94.5 | -0.0398767 |
| 99 | -0.0395075 |
| 103.5 | -0.0388948 |
| 108 | -0.0380423 |
| 112.5 | -0.0369552 |
| 117 | -0.0356403 |
| 121.5 | -0.0341056 |
| 126 | -0.0323607 |
| 130.5 | -0.0304162 |
| 135 | -0.0282843 |
| 139.5 | -0.0259779 |
| 144 | -0.0235114 |
| 148.5 | -0.0208999 |
| 153 | -0.0181596 |
| 157.5 | -0.0153073 |
| 162 | -0.0123607 |
| 166.5 | -0.00933781 |
| 171 | -0.00625738 |
| 175.5 | -0.00313836 |
| 180 | 0 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Segment force x | 0 | N |
| Segment force y | 0 | N |
| Segment force z | -0.04 | N |
| Segment force magnitude | 0.04 | N |
| Conventional charge crossing per second | 4 | C/s |
The transverse segment component controls force; parallel and antiparallel orientations give exact zero.
I L cross B uses conventional-current direction, not electron drift direction. Here L=(Lcosθ,Lsinθ,0) and B=(B,0,0), so Fz=−ILBsinθ. Reversing current reverses force. In a closed loop inside a spatially uniform field, opposite segments cancel net force while separated forces can still make a torque; one-segment force is not the whole-loop resultant.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The transverse segment component controls force; parallel and antiparallel orientations give exact zero.
I L cross B uses conventional-current direction, not electron drift direction. Here L=(Lcosθ,Lsinθ,0) and B=(B,0,0), so Fz=−ILBsinθ. Reversing current reverses force. In a closed loop inside a spatially uniform field, opposite segments cancel net force while separated forces can still make a torque; one-segment force is not the whole-loop resultant.
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