Faraday's Law EMF Calculator
Calculate induced EMF from changing magnetic flux using Faraday's law.
Changing Magnetic Flux Produces Electromotive Force
Faraday’s law says an induced emf appears whenever magnetic flux linkage through a circuit changes with time. For N identical turns, ε=−N dΦB/dt. Flux through a flat loop in a uniform field is ΦB=BAcosθ, so induction can result from changing field strength, loop area, orientation, or any combination of these.
The minus sign is Lenz’s law: the induced current acts in a direction whose magnetic effect opposes the change in flux. It is not a claim that emf magnitude is negative; polarity depends on the chosen loop orientation and sign convention.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| ε | Induced emf | V. |
| N | Number of turns | Dimensionless; flux linkage scales with turns. |
| ΦB | Magnetic flux | Wb=T·m². |
| θ | Angle between B and area normal | Controls the normal field component. |
A large flux can produce zero emf if it is constant. Induction depends on the rate of change of flux linkage, which is why rapidly changing fields or motion can create large voltages.
Flux linkage is the key induction quantity. Doubling the number of identical turns doubles the induced emf for the same rate of flux change. If magnetic flux is constant in time, the induced emf must be zero even when the flux itself is large.
Worked Examples
Common Mistakes
Faraday’s law depends on dΦ/dt, not field magnitude alone.
Flux uses BAcosθ where θ is between B and the surface normal.
The induced direction opposes the change in flux, which is essential for signs in circuits and generators.
Frequently Asked Questions
Formula Explorer connections
Interpretation: This relationship connects magnetic fields, moving charge, flux, induction or electromagnetic material response. Assumption: Specify field direction and sign convention. Uniform fields, linear materials, negligible edge effects or sinusoidal steady state may be assumed.