Mutual Inductance Calculator
Calculate mutual inductance, coupling coefficient, and induced EMF between two coupled inductors.
How One Coil Induces Voltage in Another
Mutual inductance measures how effectively a changing current in one circuit creates magnetic flux linkage in a second circuit. If current I1 changes, the linked flux through coil 2 changes and Faraday’s law produces an induced emf ε2=−M dI1/dt. The minus sign expresses Lenz’s law: the induced effect opposes the change that created it.
For two inductors with self-inductances L1 and L2, M=k√(L1L2), where the coupling coefficient 0≤k&le1 describes how much of one coil’s magnetic flux links the other. Geometry, spacing, orientation, and magnetic core material strongly influence k.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| M | Mutual inductance | H; strength of magnetic coupling between two circuits. |
| k | Coupling coefficient | Dimensionless, from 0 for no coupling to 1 for ideal complete coupling. |
| dI/dt | Current change rate | A/s; faster current changes induce larger voltage. |
A large M does not by itself guarantee high efficiency; winding resistance, core losses, leakage flux, and frequency effects also matter. In transformer analysis, dot convention determines the relative polarity of induced voltages.
Mutual inductance cannot exceed √(L1L2) for passive coupled coils. The coupling coefficient k=M/√(L1L2) should lie between 0 and 1. A computed k above 1 indicates inconsistent inductance data or a unit-conversion error.
Worked Examples
Common Mistakes
For passive coupled inductors, the magnitude of coupling coefficient cannot exceed 1. Values above 1 violate M²≤L₁L₂.
Magnitude calculations may omit the sign, but circuit polarity depends on winding orientation and the dot convention.
Induced emf depends on dI/dt. A steady DC current can establish flux but produces no continuing transformer emf after transients settle.
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.