A millihenry (mH) is one-thousandth of a henry, measuring an inductor's ability to store energy in a magnetic field and resist changes in electrical current. When you place an mH-rated component into a circuit, it fundamentally changes the current slew rate and the frequency-dependent impedance, acting as a bottleneck for high-frequency AC while letting DC pass unimpeded. If you are reading this because you are staring at a schematic calling for a '4.7mH choke' or a '1.5mH crossover coil', this guide will give you the exact math, the physical constraints, and the specific part numbers you need to finish the build.
The Physics of a Millihenry (Without the Fluff)
To understand what a millihenry actually does on your bench, think of an inductor like a mechanical flywheel connected to a motor. When you apply voltage (torque), the flywheel (inductor) resists spinning up immediately; it takes time to build momentum (magnetic field). Once it is spinning, if you try to cut the power, the flywheel's inertia keeps it turning, generating its own voltage to keep the current flowing.
In electrical terms, this inertia is inductance. A 1 mH inductor will generate a back-EMF of 1 volt if the current through it changes at a rate of 1 ampere per second ($V = L \frac{di}{dt}$). In practical circuits, this means mH-rated components are used to smooth out jagged current ripples in power supplies, block high-frequency noise in EMI filters, and divide audio frequencies in speaker crossovers.
Worked Example: Calculating a 1.59 mH Woofer Crossover
Let us look at a real-world scenario where millihenries are the primary design constraint: building a passive 2nd-order low-pass audio crossover for an 8-ohm woofer. You want to cut off frequencies above 800 Hz to protect the woofer from distortion.
The formula for the inductor in a 2nd-order Butterworth low-pass filter is:
$L = \frac{R}{2 \pi f_c}$
- $R$ (Nominal Speaker Impedance) = 8 Ω
- $f_c$ (Target Cutoff Frequency) = 800 Hz
- $\pi$ ≈ 3.14159
Plugging in the real values:
$L = \frac{8}{2 \times 3.14159 \times 800}$
$L = \frac{8}{5026.5}$
$L = 0.001591 \text{ Henries}$
Converting to millihenries, we get 1.59 mH. If you install a 1.59 mH inductor in series with your woofer, it will present an impedance of roughly 8 Ω at 800 Hz, creating your -3dB crossover point. If you mistakenly grab a 1.59 microhenry (µH) part from the bin, the crossover frequency will shift to roughly 800 kHz, effectively removing the filter and blowing your speaker.
Where You Meet mH Ratings in Practice
While microhenries (µH) dominate high-frequency switch-mode power supplies (SMPS), millihenries rule the low-frequency and high-energy domains. Here is where you will encounter them:
- Audio Crossovers: Woofer and subwoofer low-pass filters typically require 1.0 mH to 15.0 mH inductors to handle high audio wattage without saturating.
- EMI Common-Mode Chokes: Input filters on mains-powered equipment use 10 mH to 100 mH toroidal chokes to block high-frequency switching noise from escaping back into the grid.
- Low-Frequency Ballasts and Transformers: Fluorescent lighting and legacy motor controls rely on high-mH inductance to limit AC current flow at 50/60 Hz.
- Sensor and Relay Coils: The physical coils inside heavy-duty contactors and industrial relays often measure in the tens or hundreds of millihenries.
The Inductor Selection Decision Tree
Knowing the mH value is only half the battle. You must also select the correct core material and current rating. Use this decision path to terminate your part selection.
| Application | Priority Spec | Core Material | Concrete Pick (Example) |
|---|---|---|---|
| Audio Crossovers (High Fidelity) | Low DCR, Zero Saturation | Air Core or Foil | Dayton Audio 1.5mH Air Core (Part #255-030) |
| Mains EMI Filtering | High Common-Mode Impedance | Nanocrystalline / Ferrite | Bourns 2100-RC Series (e.g., 10mH) |
| Low-Freq Power Filtering (<10kHz) | High Saturation Current (Isat) | Powdered Iron / Kool Mµ | Coilcraft DO3316P Series |
| Signal Line Chokes (Audio/Data) | Small Footprint, Low Current | Ferrite Drum | Murata 1400 Series (e.g., 2.2mH) |
The Great Unit Confusion: mH vs. mAh vs. µH
Because electronics relies heavily on SI prefixes, the 'mH' designation is a frequent victim of misreading and typo-induced failures. Here is what people commonly confuse it with:
- mH (millihenry) vs. mAh (milliamp-hour): This is the most common beginner mistake. mH measures inductance (magnetic energy storage). mAh measures battery capacity (chemical energy storage). A 3000 mAh battery has nothing to do with a 3000 mH inductor.
- mH (millihenry) vs. µH (microhenry): A millihenry is 1,000 times larger than a microhenry. Schematics often use 'uH' instead of the Greek 'µ'. If a schematic calls for 4.7uH and you install a 4.7mH choke, your switching regulator will likely fail to start or will suffer massive transient ringing.
- Lower-case 'm' vs. Upper-case 'M': In SI units, 'm' is milli ($10^{-3}$) and 'M' is Mega ($10^6$). While a 'Megahenry' does not exist in practical electronics, confusing the prefixes in other components (like mΩ vs MΩ) is a classic bench error.
Frequently Asked Questions
Can I measure mH with a standard multimeter?
No. A standard multimeter measures DC resistance (DCR) in ohms, not inductance. To measure millihenries, you need a dedicated LCR meter (like the Keysight U1733C or a budget DE-18) that applies an AC test signal (usually 1 kHz) to calculate the reactance.
Why do audio inductors have such thick wire?
Audio crossover inductors carry the full amplifier current (often 10A to 30A peaks). If the wire is too thin, the DC Resistance (DCR) will rise, robbing the amplifier of power and altering the speaker's Q-factor. High-end mH audio inductors use 14 AWG or even 12 AWG copper wire to keep DCR below 0.2 Ω.
Does the physical orientation of an mH inductor matter?
Yes. Inductors emit magnetic fields. If you place two high-mH inductors close together on a PCB or in a speaker cabinet, their fields will couple, causing crosstalk and altering the effective inductance. Always mount them at 90-degree angles to one another and space them at least one core-diameter apart.
For deeper reading on inductor behavior and filter design, consult the inductor theory chapters on All About Circuits or review practical component application notes via Electronics Tutorials. When in doubt, trust the datasheet's $I_{sat}$ and DCR curves over the nominal mH stamp on the casing.






