12.5
V
1.25
A
1,250
mA
15.625
W
0.25
Wb/s
12.5
Wb/s
-1
12.5
V
1.25
A
1,250
mA
15.625
W
0.25
Wb/s
12.5
Wb/s
-1
The Lenz's Law Calculator computes the induced EMF, the resulting current, power dissipation, and the direction of induced current when magnetic flux through a coil changes over time. Lenz's law, which is embedded in the negative sign of Faraday's law, states that the induced current always flows in a direction that opposes the change in flux that produced it.
This principle is crucial for understanding electromagnetic braking, eddy current damping, back-EMF in motors, and the energy conservation aspects of electromagnetic induction. By calculating both the magnitude and direction of induced quantities, this tool provides a complete picture of the induction phenomenon.
Starting from Faraday's law:
$$\varepsilon = -N\frac{\Delta\Phi}{\Delta t}$$
The magnitude of the induced EMF is:
$$|\varepsilon| = N\frac{|\Delta\Phi|}{\Delta t}$$
The induced current in a closed circuit of resistance $$R$$ follows from Ohm's law:
$$I = \frac{|\varepsilon|}{R} = \frac{N|\Delta\Phi|}{R \cdot \Delta t}$$
The power dissipated in the resistance is:
$$P = I^2 R = \frac{\varepsilon^2}{R} = \frac{N^2(\Delta\Phi)^2}{R(\Delta t)^2}$$
Lenz's law determines the current direction: if the external flux through the coil is increasing ($$\Delta\Phi > 0$$), the induced current flows in the direction that creates a magnetic field opposing the increase (counterclockwise when the flux vector points toward you, by the right-hand rule). If the flux is decreasing, the current flows to support the diminishing field (clockwise in the same viewing convention).
This opposition is not merely a convention — it is a direct consequence of energy conservation. Without Lenz's law, the induced current would reinforce the flux change, creating a runaway process that generates energy from nothing. Instead, work must be done against the opposing force to maintain the flux change, and this mechanical work is converted to electrical energy dissipated as heat in the resistance.
Induced EMF is the voltage generated by the changing flux. Induced Current is the EMF divided by the circuit resistance — lower resistance means more current for the same EMF. Power Dissipated is the energy per second converted to heat in the resistance, equaling the mechanical power input needed to sustain the flux change. Current Direction tells you which way the current flows based on whether the flux is increasing or decreasing, following the right-hand rule convention.
Inputs
Results
A magnet pushed toward a 50-turn coil (ΔΦ = +0.005 Wb in 20 ms) induces 12.5 V and 1.25 A counterclockwise current that repels the magnet.
Inputs
Results
Same magnitudes as approach, but the current direction reverses — now clockwise to attract the departing magnet and oppose the flux decrease.
Lenz's law ensures the induced current opposes the cause of induction. This opposition means external work must be done to change the flux, and that work equals the electrical energy produced. Without this opposition, perpetual motion would be possible.
Very low resistance means very large induced current, which creates a strong opposing magnetic field. This is the principle behind electromagnetic braking — a conductor moving through a magnetic field experiences strong retarding forces when its resistance is low.
When a conductor moves through a magnetic field, eddy currents are induced that (by Lenz's law) oppose the motion. This creates a braking force proportional to speed, used in roller coasters, train brakes, and laboratory balances.
A spinning motor generates an EMF (by Faraday's law) that opposes the applied voltage (by Lenz's law). This back-EMF limits the current drawn by the motor. At startup (no spinning), there is no back-EMF, so startup current is very high.
Yes. The 'clockwise' or 'counterclockwise' designation depends on the viewing orientation and the chosen positive flux direction. The physics is unambiguous: the induced B-field always opposes the flux change.
Yes. Determine whether flux is increasing or decreasing, then use the right-hand rule to find which current direction would oppose that change. The terminal through which this current exits is the positive terminal of the induced EMF.
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