30
mH
25
mH
—
Ω
30
mH
25
mH
—
Ω
Series inductors add directly: L_total = L1 + L2 + L3 + ... when there is no magnetic coupling between them. This is the simplest inductor configuration and mirrors series resistors in its direct addition rule. The total inductance determines the combined energy storage, impedance, and filtering characteristics of the series inductor network.
However, when inductors are physically close, their magnetic fields interact through mutual inductance (M). For two coupled inductors in series, the total inductance is: L_total = L1 + L2 ± 2M. The plus sign applies when the inductors are wound to aid each other (current enters both at dotted terminals), increasing total inductance. The minus sign applies when they oppose each other, decreasing total inductance. This mutual coupling effect is the principle behind coupled inductors, transformers, and common-mode chokes.
Series inductors are used extensively in filtering applications. A series inductor in a power supply filter presents high impedance to AC ripple while passing DC load current with minimal voltage drop (limited only by the wire's DC resistance, DCR). Multiple series inductors create a cascaded filter for higher ripple attenuation. The series impedance XL = 2πfL increases with frequency, providing better filtering at higher harmonic frequencies.
In RF circuit design, series inductors form part of impedance matching networks. An L-network for matching a 50 Ω source to a high-impedance antenna typically uses a series inductor and a shunt capacitor. The series inductor value is chosen for proper impedance transformation at the target frequency.
Common-mode chokes are a practical application of magnetically coupled series inductors. Two coils wound on the same ferrite toroid core are connected in series with the supply and return conductors. For differential (normal) current, the fluxes cancel (opposing configuration), giving very low impedance. For common-mode noise, the fluxes add (aiding configuration), giving high impedance that suppresses EMI. The mutual inductance M equals nearly L1 = L2 for a tightly coupled common-mode choke, making differential impedance ≈ 0 while common-mode impedance = 2L.
This calculator provides both the uncoupled series inductance (L1 + L2 + L3) and the two-inductor coupled inductance (L1 + L2 ± 2M), along with inductive reactance at the specified frequency — a complete toolkit for inductor network analysis.
Uncoupled series inductance: L_total = L1 + L2 + L3 (direct addition, assumes M = 0). Coupled (L1+L2 only): L_total = L1 + L2 + 2M (positive M = aiding, negative M = opposing). Reactance XL = 2πf × L_total (no-mutual case, converting mH to H). Enter M = 0 for uncoupled inductors.
Series inductance is always greater than the largest individual inductor (without coupling). With aiding mutual inductance, total is even larger. With opposing mutual inductance, total may be less than either individual value. Higher total inductance means higher reactance at given frequency — better filtering but more voltage drop across DCR at high currents.
Inputs
Results
Two 100 mH chokes with M = 90 mH in aiding configuration give 380 mH — near the theoretical maximum of 400 mH (when M = L). At 150 kHz (typical EMI frequency): XL = 188 kΩ, providing excellent common-mode attenuation.
Inputs
Results
47 + 22 + 10 mH in series (no coupling) = 79 mH with XL = 24.8 kΩ at 50 kHz — high impedance to switching ripple while allowing DC load current through DCR.
The dot convention marks the terminal of each winding where current entering produces flux in the same direction. When current enters at both dotted terminals simultaneously, fluxes add (aiding). When current enters one dotted and one non-dotted terminal, fluxes oppose. Use the dot convention consistently when connecting inductors in series or designing transformers.
The coupling coefficient k = M / √(L1 × L2) ranges from 0 (no coupling) to 1 (perfect coupling). k = 0.99+ for tightly wound transformers. k = 0.1–0.5 for loosely coupled coils. k affects the bandwidth of coupled resonators in bandpass filters — higher k gives wider bandwidth but flatter passband.
Most standard multimeters don't measure inductance. Use an LCR meter (impedance analyzer) which applies a known frequency AC signal and measures V/I phase relationship to extract L, C, and R. Measure at the intended operating frequency for most accurate results. At DC, an inductor measures only its DC resistance (DCR).
As DC current through a ferrite-core inductor increases, the core approaches magnetic saturation — the incremental inductance drops rapidly. Datasheets specify L vs. DC bias current curves. Always select inductors whose saturation current (where L drops to 70–80% of nominal) exceeds the peak current in your application, including ripple current.
From V = L × dI/dt, rapidly interrupting current (high dI/dt from a fast switch) across an inductor generates high voltage (V = L × ΔI/Δt). A 10 mH inductor with 5 A interrupted in 1 µs generates 50,000 V — a destructive spike. Snubber circuits (RC or diode clamps) limit dI/dt or provide current commutation paths to prevent overvoltage.
A ferrite bead is a lossy inductor — its impedance at high frequencies comes primarily from resistance (energy absorption) rather than reactance (energy storage). Unlike a capacitor or resonant inductor, a ferrite bead absorbs and dissipates EMI as heat rather than reflecting it. This prevents EMI from being re-emitted elsewhere in the circuit — making ferrite beads ideal for power rail filtering at high frequencies (>10 MHz).
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