Inductive Reactance Calculator - XL = 2πfL Coil Reactance Solver

Use this inductive reactance calculator to solve XL = 2π f L for any coil with H, mH, µH, nH inductance and Hz, kHz, MHz, GHz frequency, plus auto Ω output.

Inductive Reactance Calculator

Self-inductance of the coil in the selected prefix. Converted to henries before XL = 2π f L.

Unit prefix of the inductance. Auto-converted to henries before the formula runs.

Signal frequency applied to the inductor in the selected prefix. Converted to hertz before XL = 2π f L.

Unit prefix of the frequency. Auto-converted to hertz before the formula runs.

Results

Inductive Reactance (XL)
0
Inductance 0H
Frequency 0Hz
Angular Frequency (ω) 0rad/s
Period (T = 1 / f) 0s
Wavelength (c / f) 0m

What Is Inductive Reactance?

An inductive reactance calculator solves XL = 2π f L for any coil in an AC circuit, taking the self-inductance in henries and the signal frequency in hertz and returning the magnitude of the coil's AC opposition in ohms, so an engineer or student can size a choke or filter without re-deriving the equation. The formula pairs with the capacitive-reactance page: a capacitor blocks DC and passes high frequencies, while an inductor blocks them.

  • AC circuit homework: Find the XL a textbook problem gives for an inductor and a chosen frequency so the rest of the circuit can be solved.
  • Audio crossover inductor sizing: Estimate the reactance of a coil at a 20 Hz to 20 kHz audio band so the corner frequency of the low-pass filter is known.
  • Switching supply choke selection: Check the XL of a power inductor at the 50 kHz to 500 kHz switching frequency when sizing the ripple current.
  • RF choke and EMI filter design: Convert a chosen inductance into a reactance at RF so a matching network can be designed.

The calculator assumes an ideal inductor with a purely reactive AC impedance, so the printed XL is the magnitude of the impedance. Real coils add a small series resistance (DCR) and a parallel parasitic capacitance that bend the impedance away from the formula above the self-resonant frequency; check the datasheet SRF for RF work.

Reactive opposition is what separates inductors from resistors in AC analysis: a resistor dissipates real power as heat, while an ideal inductor stores energy in its magnetic field during part of every cycle and returns it during the next quarter cycle, so the average real power is zero.

A coil and a capacitor in the same AC circuit react in opposite ways, and the Capacitive Reactance Calculator solves the matching Xc = 1 / (2π f C) for the capacitor half of the same analysis.

How Inductive Reactance Works

The inductive reactance calculator applies the AC-circuit equation XL = 2π f L to the inductance and frequency the user enters, with automatic conversion of the chosen unit prefixes into the SI base units the formula expects.

XL = 2π · f · L
  • L: Self-inductance of the coil in henries (H). Calculator accepts H, mH, µH, or nH prefixes and converts to henries before the formula runs.
  • f: Frequency of the AC signal applied to the inductor in hertz (Hz). Calculator accepts Hz, kHz, MHz, or GHz prefixes and converts to hertz before the formula runs.
  • π: The mathematical constant pi ≈ 3.14159265358979. Used to convert between angular frequency ω (rad/s) and cyclic frequency f (Hz).
  • XL: Inductive reactance in ohms (Ω). Auto-prefixed to mΩ, Ω, kΩ, or MΩ so the printed value stays readable across nH inductors at GHz to H inductors at 50 Hz.

The formula is the magnitude of the complex impedance Z = j ω L of an ideal inductor, which is why XL rises linearly with both frequency and inductance and why an inductor looks like a short at DC and an open at high frequencies. Equivalently XL = ω L with ω = 2π f, and the inductive reactance calculator displays ω next to XL for reuse in a Bode plot.

Once XL is known, the next step is the AC voltage across the coil at a given current, and V = I · XL holds in phasor form just as it does for a resistor, so the calculator output drops into any AC solver that accepts V, I, and Z in phasor form.

1 mH inductor at 1 kHz returns XL ≈ 6.283 Ω

Inductance = 1 mH, frequency = 1 kHz

L = 1e-3 H, f = 1000 Hz, so XL = 2π × 1000 × 1e-3 = 6.2831853 Ω

XL ≈ 6.283 Ω

A small iron-core inductor in the audio band has only a handful of ohms of reactance at 1 kHz, which is why an audio crossover coil typically uses millihenries.

According to HyperPhysics, the frequency dependent impedance of an inductor is called inductive reactance and equals angular frequency times inductance.

According to OpenStax, the inductive reactance of an ideal inductor at angular frequency ω is XL = ω L = 2π f L, where L is the inductance in henries and f is the signal frequency in hertz.

Once XL is known, the next step is the AC voltage across the coil at a given current, and the Ohm's Law & Basic Circuit Calculator handles V = I · Z for any voltage, current, or impedance on the same circuit.

Key Concepts Explained

Four ideas make the result panel easier to read: the role of frequency, the linear scaling with inductance, the short-circuit behavior at DC, and the 90° phase lag of inductor voltage.

Frequency dependence

XL scales linearly with f. Doubling the signal frequency doubles the reactance on the same coil, which is why a small choke that looks like a wire at 1 kHz looks like several hundred ohms at 1 MHz.

Linear scaling with inductance

XL scales linearly with L. Doubling the inductance doubles the reactance at the same frequency, which is why an audio crossover uses millihenries and an RF bias tee uses microhenries around the same formula.

Short circuit at DC

As f approaches 0, XL approaches 0. That is why an inductor passes DC while blocking AC, and why the same coil that resists 1 MHz by thousands of ohms looks almost like a wire at 60 Hz to a power supply.

90° voltage lead

In a pure inductor, the voltage leads the current by 90° (the current lags the voltage by 90°), which is what makes XL behave differently from resistance even when the magnitudes in ohms are similar.

The angular frequency ω = 2π f in rad/s is the form some sources use, with XL = ω L; the calculator displays ω alongside XL so the same value can be reused in a Bode plot or a phasor diagram. The same L that sets XL also sets the L/R time constant τ = L / R for a DC RL circuit.

The same RL time constant τ = L / R that this calculator hints at is the dual of the RC time constant τ = R C, and the Capacitor Charge Time Calculator pairs that C with a resistance and a voltage threshold to estimate the finite charge or discharge time on the same kind of circuit.

How to Use This Calculator

Type an inductance, pick the prefix, type a frequency, pick the prefix, and read XL in the ohm prefix the calculator picks.

  1. 1 Enter the inductance: Type the coil value and pick H, mH, µH, or nH as the unit prefix. The calculator converts the value to henries before the formula runs.
  2. 2 Enter the frequency: Type the signal frequency and pick Hz, kHz, MHz, or GHz as the unit prefix. The calculator converts the value to hertz before the formula runs.
  3. 3 Read XL: Read the XL result in the auto-selected ohm prefix (Ω, kΩ, or MΩ). The supporting rows show the inductance in H, frequency in Hz, angular frequency ω, period T, and wavelength λ.
  4. 4 Rescale for the next band: Change one unit prefix at a time to move between audio, mains, switching, and RF ranges without recomputing the formula by hand.

To find the reactance of a 100 µH switching choke at 100 kHz, pick 100 µH and 100 kHz. The inductive reactance calculator returns XL ≈ 62.832 Ω, the order of magnitude for the ripple reactance on a buck converter output.

When the matching capacitor for an LC filter or a tank circuit is not yet known, the Capacitance Calculator takes the parallel-plate geometry and dielectric material and returns the C in farads that pairs with this XL.

Benefits of Using This Calculator

This calculator replaces a unit-conversion-plus-log step with a single result panel that updates as you change inputs.

  • No re-derivation of XL = 2π f L: Stops you from retyping the AC-circuit formula every time the frequency or inductance changes - the form takes the inputs, the result panel takes the arithmetic.
  • Inductance prefix library: Covers H, mH, µH, and nH so datasheet values drop in without manual conversion to henries.
  • Frequency prefix library: Covers Hz, kHz, MHz, and GHz so the form handles audio, mains, switching, and RF bands.
  • Auto-selected ohm prefix: Picks mΩ, Ω, kΩ, or MΩ so the printed XL stays readable from nH RF chokes at GHz to H chokes at 50 Hz.

The unit-prefix libraries keep the form usable straight from a coil datasheet, and the auto-selected ohm prefix keeps the inductive reactance calculator result panel readable across ten orders of magnitude.

When the LC network uses several capacitors to set its resonant frequency, the Capacitors in Series Calculator reduces the C ladder to a single equivalent capacitance so the resonant frequency f = 1 / (2π √(L C)) pairs cleanly with this L.

Factors That Affect Your Results

Two inputs drive every number: the inductance the user picks and the frequency of the AC signal applied to the coil.

Inductance (L)

XL scales linearly with L. Doubling the inductance doubles the reactance at the same frequency, while a tenfold drop in inductance cuts XL by a factor of ten on the same signal.

Frequency (f)

XL scales linearly with f. Doubling the frequency doubles the reactance on the same coil, which is why a 1 mH inductor looks like a wire at 60 Hz and like several kilohms at 1 MHz.

Angular frequency (ω)

ω = 2π f converts cyclic frequency to radians per second, and some textbooks write the formula as XL = ω L; the calculator displays ω next to XL so the same value can be reused in a Bode plot.

Period (T = 1 / f)

The period in seconds is the time of one AC cycle, useful when comparing the inductor L / R time constant to the line cycle in a switching supply or a rectified DC feed.

  • The textbook XL = 2π f L assumes an ideal inductor with no parasitic resistance or capacitance; near and above the coil self-resonant frequency, parasitic capacitance dominates and the real impedance deviates from the formula.
  • The formula assumes a single-tone sinusoidal signal. A square wave has harmonics at higher frequencies where the reactance differs, so re-run the calculator at the dominant harmonic for non-sinusoidal inputs.

The inductive reactance calculator rejects zero or negative values for inductance and frequency because both make the formula undefined. When XL is below 1 Ω, the auto-prefix moves to mΩ so the small reactance of small RF chokes at high frequency stays readable.

According to NIST CODATA, the speed of light in vacuum is exactly 299,792,458 m/s, which the calculator uses to convert the chosen frequency into the wavelength readout.

When a printed reactance is needed but the geometry is what is actually known, the Capacitor Calculator works the other direction and returns the capacitance that pairs with a chosen L to hit a target resonant frequency.

Inductive reactance calculator solving XL = 2π f L for any coil with H, mH, µH, nH inductance and Hz, kHz, MHz, GHz frequency units
Inductive reactance calculator solving XL = 2π f L for any coil with H, mH, µH, nH inductance and Hz, kHz, MHz, GHz frequency units

Frequently Asked Questions

Q: What is inductive reactance?

A: Inductive reactance is the magnitude of the AC impedance of an ideal inductor, in ohms. It equals XL = 2π f L, where f is the signal frequency in hertz and L is the inductance in henries, and it rises as either the frequency or the inductance rises.

Q: How do you calculate inductive reactance from inductance and frequency?

A: Take the inductance L in henries, multiply by the frequency f in hertz, then multiply the result by 2π. With L = 1 mH and f = 1 kHz, the reactance is 2π × 1000 × 1e-3 ≈ 6.283 Ω, the right value for a small audio-crossover coil at a 1 kHz crossover frequency.

Q: What is the formula XL = 2π f L?

A: XL = 2π f L is the textbook formula for inductive reactance. L is the inductance in henries, f is the signal frequency in hertz, and the result XL is the reactance in ohms. The same formula can be written XL = ω L using angular frequency ω = 2π f in radians per second.

Q: How does inductive reactance change with frequency?

A: Inductive reactance rises linearly with frequency. Doubling the signal frequency doubles the reactance on the same coil, which is why an inductor that looks like a wire at DC looks like thousands of ohms at RF, and why small RF chokes are usually sized in microhenries rather than millihenries.

Q: What is the inductive reactance of a 1 mH inductor at 1 kHz?

A: A 1 mH inductor at 1 kHz has XL = 2π × 1000 × 1e-3 ≈ 6.283 Ω. This is the order of magnitude used when sizing an audio crossover inductor or a small line-frequency filter, where the impedance of the coil at the band of interest sets the corner frequency of the network.

Q: Why does an inductor pass DC but block AC differently from a capacitor?

A: Because XL = 2π f L tends to zero as f tends to zero, an inductor looks like a short circuit at DC and an increasingly high impedance at higher frequencies, while a capacitor does the opposite. Together they form the LC low-pass and high-pass filters used in crossovers, switching supplies, and RF matching networks.