Inductor Series and Parallel Calculator

This online tool computes the total inductance of a network made of two or more coils connected in series, parallel or any mixed arrangement. Nested branches are supported and the calculator also estimates how the input current divides between branches. Use it for filter design, power supply chokes and resonant circuits to avoid manual algebra and get a clear, instant result.

👉 Add coils and connection blocks in any quantity and at any nesting level. Enter each coil’s value and unit (nH, µH, mH, H) and specify the input current for branch current analysis.

Calculation formulas

Series connection

$$L_{\text{eq}} = L_1 + L_2 + \dots + L_n$$

Parallel connection

$$\frac{1}{L_{\text{eq}}} = \frac{1}{L_1} + \frac{1}{L_2} + \dots + \frac{1}{L_n}$$

Simple example

Three coils: 1.8 mH, 2.9 mH and 4.7 mH connected in series.

$$L_{\text{eq}} = 1.8 + 2.9 + 4.7 = 9.4\ \text{mH}$$

If the same coils are connected in parallel

$$\frac{1}{L_{\text{eq}}} = \frac{1}{1.8} + \frac{1}{2.9} + \frac{1}{4.7} \approx 1.11315 $$

$$L_{\text{eq}} \approx 0.898\ \text{mH} $$

Compound example

Coils: 3.9 mH, 5.1 mH and 9.6 mH. The 3.9 and 5.1 mH coils are in parallel; that branch is in series with 9.6 mH.

Parallel branch

$$ L_{\parallel} = \frac{1}{\frac{1}{3.9}+\frac{1}{5.1}} \approx 2.210\ \text{mH}$$

Total series with 9.6 mH

$$ L_{\text{eq}} = 2.210 + 9.6 = 11.810\ \text{mH} $$

Units of inductance

Name Symbol Value in henries
Henry H 1
Millihenry mH 10⁻³ H
Microhenry µH 10⁻⁶ H
NanoHenry nH 10⁻⁹ H

Features

  • Build networks of unlimited complexity with nested series and parallel blocks.
  • Automatic calculation of equivalent inductance and branch current distribution.
  • Text and ASCII representations of the network for quick inspection.
  • Option to download calculation results as a plain text file.

In parallel the total inductance is always lower than the smallest branch value, which is useful for HF filter design. Series connection raises total inductance while current remains the same through each coil. For mixed networks consider parasitic series resistance and stray capacitance; these factors matter above a few hundred kilohertz. For precise models use measured coil data rather than nominal values.

Further reading

  1. The Art of Electronics, Paul Horowitz and Winfield Hill — practical reference for component behavior and circuit design.
  2. Practical Electronics for Inventors, Paul Scherz and Simon Monk — hands-on coverage of components and circuits.
  3. Manufacturer application notes from Coilcraft, TDK and Murata — measurement and modeling guidance for inductors.
David Parry

David Parry — Senior Engineering Analyst

Specializing in electronics and physics-based simulations with 20+ years of engineering experience. David ensures the mathematical and physical accuracy of the tools at ProCalcLab.

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