Faraday's law of induction states that the oriented electromotive force around a closed material circuit is minus the rate of change of its linked magnetic flux:
The surface orientation and circuit direction obey the right-hand rule. The minus sign expresses Lenz's law: the induced electric current, when allowed to flow, produces a magnetic field opposing the change of linked magnetic flux. For a stationary circuit this reduces to .
The source's “Lorenz force” is the Lorentz force, . A wire element of cross-section contains carriers of charge with drift velocity . Adding their magnetic forces and using gives
for a straight wire in a uniform magnetic field. The length vector follows conventional electric current, irrespective of the carrier sign.
For the unlabelled upward-motion request, define down the slope, across the rails and out of their plane. Choose the vertical magnetic field as . An electric current across the bar in direction gives a horizontal magnetic force . The other forces are weight and the rail normal force . Uniform upward velocity requires
Consequently
Each symmetric rail supplies half of . The electric current must make point horizontally toward the uphill side; for the coordinates just defined it flows along . Reversing the vertical magnetic field reverses this current direction. The external supply must maintain that electric current against the motional electromotive force during ascent. For , no finite horizontal magnetic force can support uniform motion along the vertical rails.

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