Inductive Reactance Calculator

Calculate inductive reactance X_L = 2πfL, impedance, phase angle, and Q factor. Frequency response table shows how inductors behave across frequencies.

Use plain numbers: 1000 for 1 kHz, 1000000 for 1 MHz
Hz
Wire resistance + load resistance
Ω
V
Inductive Reactance (X_L)
3.7699 Ω
X_L = 2πfL = 2π × 60 × 1.000e-2
Total Impedance (Z)
50.1419 Ω
Z = √(R² + X_L²) = √(50² + 3.77²)
Phase Angle
4.31°
Current lags voltage by 4.3°
Current
2.3932 A
I = V/Z = 120/50.14
Power Factor
0.9972
cos(4.3°) = R/Z
Q Factor
0.08
Q = X_L/R — Low Q (lossy)
Time Constant (τ)
0.2000 ms
τ = L/R
Phase Angle Indicator
4.3° (0° = resistive, 90° = purely inductive)

Reactance vs Frequency

FrequencyX_L (Ω)Z (Ω)Current (A)Phase (°)
10 Hz0.6350.002.39980.7°
50 Hz3.1450.102.39533.6°
60 Hz3.7750.142.39324.3°
100 Hz6.2850.392.38137.2°
1 kHz62.8380.301.494451.5°
10 kHz628.32630.300.190485.5°
100 kHz6.28 kΩ6.28 kΩ0.019189.5°
1 MHz62.83 kΩ62.83 kΩ0.001990.0°

Power Analysis

QuantityValueUnit
Real Power (P)286.3720W
Reactive Power (Q)21.5919VAR
Apparent Power (S)287.1848VA
Power Factor (PF)0.9972
Planning notes, formulas, and examples

About the Inductive Reactance Calculator

Inductive reactance is the opposition an inductor presents to alternating current, and it increases linearly with frequency. The formula X_L = 2πfL shows that an inductor that passes DC freely becomes increasingly resistive to higher-frequency AC signals — the fundamental principle behind inductive filters, chokes, and impedance matching networks.

This calculator computes inductive reactance, total impedance (with series resistance), phase angle, current, power factor, quality factor (Q), and the L/R time constant. It shows how all these quantities change across a range of frequencies, making it invaluable for circuit design and analysis.

Whether you are designing a power supply filter, analyzing an RL circuit for a physics class, selecting an inductor for an RF application, or calculating the impedance of a motor winding, it gives all the key parameters. The frequency response table and power analysis give complete insight into the inductor's AC behavior across the frequency range that matters for your design.

When This Page Helps

AC circuit analysis with inductors requires combining reactance and resistance as complex numbers to find impedance, then deriving phase angle, power factor, and current. This calculator does it all in one step, plus shows the frequency-dependent behavior that is central to filter and circuit design. The Q factor output is especially useful for resonant circuit design.

How to Use the Inputs

  1. Enter the inductance value and select the unit (H, mH, or μH).
  2. Enter the operating frequency in Hz.
  3. Enter the series resistance (inductor DCR + any external resistance).
  4. Enter the applied voltage to compute current and power.
  5. Read reactance, impedance, phase angle, current, power factor, and Q from the output cards.
  6. Review the frequency response table to see how the inductor behaves at different frequencies.
  7. Check the power analysis table for real, reactive, and apparent power.
Formula used
Inductive Reactance: X_L = 2πfL Impedance (RL series): Z = √(R² + X_L²) Phase Angle: φ = arctan(X_L / R) Quality Factor: Q = X_L / R = 2πfL / R Time Constant: τ = L / R Where: f = frequency (Hz) L = inductance (H) R = resistance (Ω)

Example Calculation

Result: X_L = 3.77 Ω, Z = 50.14 Ω

A 10 mH inductor at 60 Hz: X_L = 2π × 60 × 0.01 = 3.77 Ω. With 50 Ω resistance, Z = √(50² + 3.77²) = 50.14 Ω. The phase angle is arctan(3.77/50) = 4.3°, nearly resistive. At 120V, the current is 2.39 A.

Tips & Best Practices

  • At low frequencies, X_L is small and the inductor acts like a short circuit; at high frequencies it acts like an open circuit.
  • The Q factor determines how selective or lossy the inductor is — higher Q means sharper resonance and less loss.
  • Inductor DC resistance (DCR) is critical for Q calculations; always include it in the series resistance.
  • Inductive reactance is the dual of capacitive reactance (X_C = 1/(2πfC)) — they cancel each other at resonance.
  • The L/R time constant tells you how quickly current builds up when DC is applied; 5τ to reach ~99% of final value.
  • For RF applications, self-resonant frequency limits the useful range of an inductor — above SRF, it behaves like a capacitor.

Inductors in AC Circuits

When AC voltage is applied to an inductor, the current lags the voltage by up to 90°. This phase relationship is the basis of inductive reactance. In a pure inductor (no resistance), all energy is stored in the magnetic field during one quarter cycle and returned to the circuit during the next. Adding resistance creates a complex impedance that determines both the magnitude and phase of the current.

Filter Design Applications

Inductors combined with capacitors and resistors form the building blocks of signal filters. A series inductor blocks high-frequency signals (low-pass behavior) because X_L increases with frequency. This principle is used in power supply filtering, EMI suppression, audio crossover networks, and RF front-end circuits. The Q factor determines the sharpness of the filter's frequency response.

Inductor Selection for Power Electronics

In switch-mode power supplies, the inductor must handle both DC bias current and AC ripple. The inductance value determines ripple current magnitude, while the core material and wire gauge determine losses at the switching frequency (typically 50 kHz to 2 MHz). This calculator helps evaluate whether a candidate inductor provides sufficient impedance at the switching frequency.

Sources & Methodology

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Frequently Asked Questions

  • Inductive reactance (X_L) is the opposition an inductor provides to AC current. It increases with frequency: X_L = 2πfL. Unlike resistance, reactance does not dissipate energy — it stores and returns energy to the circuit each cycle.