Reconcile motional emf, magnetic drag and mechanical work
A moving conductor can separate charge because its mobile charges experience magnetic force. For a straight rod of length L moving perpendicular to itself and to uniform B, the emf magnitude is BLv. In a closed rail circuit this drives current; in an open rod, charges separate until the internal electric field balances magnetic deflection, without a sustained loop current.
Learning outcome: Compare speeds 1 and 2 m/s at 4 Ω, then compare resistances 4 and 8 Ω at 1 m/s. Retain current sign, drag, sustaining force and both powers. Use either the charge-force or flux-change route to check the emf magnitude.
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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With B=0.50 T, L=0.40 m, v=1.0 m/s and R=4 Ω, signed emf is −0.20 V and current −0.050 A. Magnetic drag is −0.010 N. External input is +0.010 W, matching resistor heat rate; over 5 s, 0.050 J becomes heat.
Open the experimentPredict
If speed doubles with resistance fixed, do induced current and heating power both double?
Experiment
Compare speeds 1 and 2 m/s at 4 Ω, then compare resistances 4 and 8 Ω at 1 m/s. Retain current sign, drag, sustaining force and both powers. Use either the charge-force or flux-change route to check the emf magnitude.
Close a motional-induction energy ledger
Worked teaching model · synthetic values · Sliding conducting rod length 0.40 m on ideal rails, uniform B=0.50 T along +z. Closed rectangular loop expands at constant speed under external force; no friction, self-inductance or contact resistance beyond the selected total R. Normal +z defines counterclockwise circulation as positive. Virtual only.
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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 |
|---|---|---|
| Signed loop emf | -0.2 | V |
| Signed loop current | -0.05 | A |
| Magnetic drag x force | -0.01 | N |
| External sustaining x force | 0.01 | N |
| External mechanical power | 0.01 | W |
| Resistor heating power | 0.01 | W |
| Heat generated in 5 s | 0.05 | J |
Accessible plot coordinates
| rod speed (m/s) | mechanical input = resistor heat rate (W) |
|---|---|
| 0.5 | 0.0025 |
| 0.6 | 0.0036 |
| 0.7 | 0.0049 |
| 0.8 | 0.0064 |
| 0.9 | 0.0081 |
| 1 | 0.01 |
| 1.1 | 0.0121 |
| 1.2 | 0.0144 |
| 1.3 | 0.0169 |
| 1.4 | 0.0196 |
| 1.5 | 0.0225 |
| 1.6 | 0.0256 |
| 1.7 | 0.0289 |
| 1.8 | 0.0324 |
| 1.9 | 0.0361 |
| 2 | 0.04 |
Lenz’s-law drag and resistor heating reconcile the mechanical and electrical energy accounts.
The expanding +z flux gives negative (clockwise) current. At the moving right-hand rod, clockwise current is downward, so IL×B points −x. External power Fv equals I²R. Although the microscopic magnetic force does no work on a charge, the externally driven conductor transfers mechanical energy to the circuit; a maintained speed is not free energy.
Lenz’s-law drag and resistor heating reconcile the mechanical and electrical energy accounts.
The expanding +z flux gives negative (clockwise) current. At the moving right-hand rod, clockwise current is downward, so IL×B points −x. External power Fv equals I²R. Although the microscopic magnetic force does no work on a charge, the externally driven conductor transfers mechanical energy to the circuit; a maintained speed is not free energy.
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Explain which omitted energy terms would be required if the rod slowed down rather than moving at prescribed constant speed.
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