Compute the total equivalent inductance (Leq) for parallel-connected inductors. Understand the reciprocal sum rule, view interactive circuit diagram, and explore real‑world applications in power electronics, EMI filters, and resonant circuits.
When inductors are connected in parallel, the total or equivalent inductance (Leq) is found using the reciprocal sum formula, analogous to resistors in parallel but with one key difference: inductors oppose changes in current. For uncoupled (magnetically independent) inductors, the rule is:
Therefore, \(L_{eq} = \left( \sum_{i=1}^{n} \frac{1}{L_i} \right)^{-1}\). The equivalent inductance is always less than the smallest individual inductance in the parallel combination — a critical fact for filter design and power distribution networks. The derivation stems from Kirchhoff's voltage law and the voltage-current relationship \(v = L \frac{di}{dt}\) in parallel branches: same voltage across each inductor, total current is the sum of branch currents.
For n parallel inductors with identical voltage v(t): \(i_k(t) = \frac{1}{L_k} \int v(t) dt\). Total current \(i_{total} = \sum i_k = \left( \sum \frac{1}{L_k} \right) \int v(t) dt\). Comparing with \(i_{total} = \frac{1}{L_{eq}} \int v(t) dt\) yields the reciprocal rule.
In multi-phase buck converters, engineers often place multiple inductors in parallel to reduce output ripple current and increase power density. For instance, two 2.2 µH inductors in parallel provide an effective 1.1 µH inductance while spreading thermal load. Our calculator helps designers quickly evaluate trade-offs between ripple current, size, and efficiency. The reciprocal formula ensures predictable performance when magnetic coupling is minimized via physical spacing.
The basic parallel formula assumes zero mutual inductance (M = 0). If inductors share a common magnetic core or are wound on the same former, mutual coupling alters the equivalent value. For mutually coupled inductors in parallel (aiding or opposing), the total inductance becomes:
\(L_{eq} = \frac{L_1 L_2 - M^2}{L_1 + L_2 \mp 2M}\) (depending on dot convention). Most practical designs avoid unintended coupling; the tool provided assumes ideal uncoupled inductors, which holds true for air-core coils or well-shielded SMD inductors placed apart.