Read induced polarity from changes in a flux record
Faraday’s law relates average induced emf to flux change: emf=−NΔΦ/Δt for N turns with the same per-turn flux. The minus sign encodes Lenz’s law: induced current, if a closed path permits it, produces a field that opposes the change in flux. It does not always oppose the original field; when the original field is decreasing, the response can support it.
Learning outcome: Capture 20 turns and ramp duration 0.20 s. Reconstruct all three interval polarities and currents. Double the turns, then separately double duration, explaining the emf and total resistor-heat changes using the declared 10 Ω assumption.
Starting recap
State coordinate axes, charge/current signs and oriented surface normals. Distinguish field from force, magnetic flux from its rate of change, and microscopic magnetic work from a full mechanical/electrical energy ledger.
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For 20 turns, area 0.010 m² and B rising from 0.10 to 0.40 T in 0.20 s, per-turn flux changes by 0.0030 Wb. The ramp emf is −0.30 V and current −0.030 A. The hold emf is zero; the equal-duration return ramp gives +0.30 V.
Open the experimentPredict
Will the induced emf be largest during the plateau where flux is largest?
Experiment
Capture 20 turns and ramp duration 0.20 s. Reconstruct all three interval polarities and currents. Double the turns, then separately double duration, explaining the emf and total resistor-heat changes using the declared 10 Ω assumption.
Infer signed emf from a piecewise-linear flux record
Worked teaching model · synthetic values · Each turn has fixed area 0.010 m², normal +z and resistance of entire coil 10 Ω. B ramps uniformly from 0.10 to 0.40 T, holds for one ramp duration, then returns uniformly to 0.10 T. Negligible self-inductance; piecewise emf is undefined at idealized slope-change instants, so intervals are reported separately.
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| Interval | Start (s) | End (s) | emf (V) | Current (A) |
|---|---|---|---|---|
| Increasing +z flux | 0 | 0.2 | -0.3 | -0.03 |
| Constant flux | 0.2 | 0.4 | 0 | 0 |
| Decreasing +z flux | 0.4 | 0.6 | 0.3 | 0.03 |
Axes rescale with settings; compare numerical values, not screen lengths across different settings. Orbit x/y use the same spatial scale within one plot. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Ramp-up signed emf | -0.3 | V |
| Hold signed emf | 0 | V |
| Ramp-down signed emf | 0.3 | V |
| Ramp current magnitude | 0.03 | A |
| Total resistor heat in both ramps | 0.0036 | J |
Accessible plot coordinates
| time (s) | flux through one turn (mWb) |
|---|---|
| 0 | 1 |
| 0.2 | 4 |
| 0.4 | 4 |
| 0.6 | 1 |
The induced emf follows the signed flux-change rate, not the instantaneous size of flux.
Normal +z defines counterclockwise as positive when viewed from +z. Rising +z flux induces clockwise current and opposing −z field; falling flux induces counterclockwise current that supports the diminishing +z field. The external agent changing the field supplies dissipated energy. Current requires the closed resistive path stipulated here.
The induced emf follows the signed flux-change rate, not the instantaneous size of flux.
Normal +z defines counterclockwise as positive when viewed from +z. Rising +z flux induces clockwise current and opposing −z field; falling flux induces counterclockwise current that supports the diminishing +z field. The external agent changing the field supplies dissipated energy. Current requires the closed resistive path stipulated here.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
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Public practice checks a specific claim. It does not establish independent mastery.
Explain why Lenz’s law opposes a change rather than always opposing the existing field, and name the energy source.
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