Inductive Reactance Calculator

Calculate inductive reactance, impedance, and phase angle for AC circuits with inductors.

Determine the opposition to alternating current flow in inductive circuits. Essential for designing filters, transformers, and AC power systems.

Examples

Click on any example to load it into the calculator.

Power Line Inductor

Power Line Inductor

Typical inductor used in power line filtering applications.

Frequency: 60 Hz

Inductance: 0.1 H

Voltage: 120 V

Resistance: 5 Ω

Audio Frequency Inductor

Audio Frequency Inductor

Inductor used in audio crossover networks and filters.

Frequency: 1000 Hz

Inductance: 10 mH

Voltage: 12 V

Resistance: 2 Ω

RF Circuit Inductor

RF Circuit Inductor

High-frequency inductor for radio frequency applications.

Frequency: 1000000 Hz

Inductance: 100 μH

Voltage: 5 V

Resistance: 0.5 Ω

Transformer Primary

Transformer Primary

Primary winding of a small power transformer.

Frequency: 50 Hz

Inductance: 2 H

Voltage: 230 V

Resistance: 15 Ω

Other Titles
Understanding Inductive Reactance: A Comprehensive Guide
Master the fundamentals of inductive reactance in AC circuits. Learn how inductors behave differently with alternating current compared to direct current, and discover practical applications in electrical engineering.

What is Inductive Reactance?

  • Core Concepts
  • AC vs DC Behavior
  • Mathematical Foundation
Inductive reactance (XL) is the opposition that an inductor presents to alternating current flow. Unlike resistance, which opposes both AC and DC equally, reactance is frequency-dependent and represents the energy storage and release characteristics of the inductor. When AC voltage is applied to an inductor, the current lags behind the voltage by 90 degrees, creating a phase difference that is fundamental to AC circuit analysis.
The Physics Behind Inductive Reactance
Inductive reactance arises from Faraday's law of electromagnetic induction. When alternating current flows through an inductor, it creates a changing magnetic field. This changing field induces a voltage (back EMF) that opposes the applied voltage, effectively resisting the current flow. The faster the current changes (higher frequency), the stronger this opposition becomes, making reactance directly proportional to frequency.
AC vs DC: Fundamental Differences
With direct current, an inductor initially opposes current flow due to the back EMF, but once the current stabilizes, the inductor behaves like a short circuit (assuming ideal conditions). In AC circuits, the current is constantly changing, so the inductor continuously opposes the current flow, creating a frequency-dependent impedance that increases with frequency.
The Reactance Formula
The fundamental formula for inductive reactance is XL = 2πfL, where XL is the reactance in ohms, f is the frequency in Hertz, and L is the inductance in Henrys. This simple equation reveals that reactance doubles when either frequency or inductance doubles, making it a linear relationship with both parameters.

Key Reactance Characteristics:

  • Frequency Dependence: Reactance increases linearly with frequency
  • Phase Relationship: Current lags voltage by 90° in pure inductive circuits
  • Energy Storage: Inductors store energy in their magnetic field
  • Power Factor: Pure inductive circuits have a power factor of 0 (no real power consumed)

Step-by-Step Guide to Using the Calculator

  • Input Parameters
  • Understanding Results
  • Practical Applications
The inductive reactance calculator provides comprehensive analysis of inductor behavior in AC circuits. By inputting frequency, inductance, voltage, and resistance, you can determine not only the reactance but also the total impedance, current flow, phase relationships, and power characteristics.
1. Frequency Input
Enter the frequency of your AC signal. Common values include 50 Hz (European power), 60 Hz (North American power), 400 Hz (aircraft power), and higher frequencies for electronics applications. The calculator accepts any positive frequency value.
2. Inductance Specification
Input the inductance value and select the appropriate unit. Large inductors (transformers, chokes) are typically measured in Henrys (H), while smaller components use milliHenrys (mH) or microHenrys (μH). Be precise with this value as it directly affects reactance.
3. Voltage and Resistance
The applied voltage determines the current flow through the circuit. The series resistance represents the internal resistance of the inductor windings and any external resistance. These values are used to calculate power dissipation and quality factor.
4. Interpreting the Results
The calculator provides multiple outputs: Inductive reactance (XL) shows the pure reactive opposition, total impedance (Z) combines reactance and resistance, current (I) shows the actual current flow, phase angle (θ) indicates the voltage-current relationship, and quality factor (Q) measures the inductor's efficiency.

Common Frequency Ranges:

  • Power Systems: 50-60 Hz (utility power)
  • Audio Systems: 20 Hz - 20 kHz (human hearing range)
  • Radio Frequency: 3 kHz - 300 GHz (communications)
  • Switching Power Supplies: 20 kHz - 1 MHz (high-frequency operation)

Real-World Applications of Inductive Reactance

  • Power Systems
  • Electronics Design
  • Filter Applications
Inductive reactance is fundamental to modern electrical and electronic systems. Understanding how inductors behave in AC circuits is essential for designing efficient power systems, electronic filters, and communication equipment.
Power Factor Correction
In industrial power systems, inductive loads (motors, transformers) create lagging power factors that reduce system efficiency. Power factor correction capacitors are used to offset inductive reactance, improving power factor and reducing energy costs. The calculator helps engineers determine the required correction.
Filter Design
Inductors are essential components in electronic filters. Low-pass filters use inductors to block high frequencies, while high-pass filters use capacitors. Band-pass and band-stop filters combine both components. The reactance calculator helps designers select appropriate component values for desired frequency responses.
Transformer Design
Transformers rely on inductive coupling between primary and secondary windings. The primary winding's inductive reactance determines the magnetizing current and affects efficiency. Designers use reactance calculations to optimize transformer performance and minimize losses.
RF and Communication Systems
In radio frequency applications, inductors are used in tuning circuits, impedance matching networks, and oscillators. The frequency-dependent nature of reactance is crucial for designing circuits that operate at specific frequencies or over frequency ranges.

Quality Factor Applications:

  • High-Q inductors (>100): Used in precision oscillators and filters
  • Medium-Q inductors (10-100): General-purpose applications
  • Low-Q inductors (<10): Power applications where efficiency is priority

Common Misconceptions and Correct Methods

  • Reactance vs Resistance
  • Power in Reactive Circuits
  • Frequency Effects
Several misconceptions surround inductive reactance and AC circuit behavior. Understanding these helps avoid design errors and improves circuit performance.
Misconception: Reactance is the Same as Resistance
While both oppose current flow, they work through different mechanisms. Resistance dissipates energy as heat, while reactance stores and releases energy. Resistance is constant regardless of frequency, while reactance varies with frequency. In AC circuits, both contribute to total impedance through vector addition.
Misconception: No Power is Consumed in Reactive Circuits
While pure reactance doesn't consume real power, real inductors have resistance that dissipates power. The apparent power (S = VI) includes both real power (P = I²R) and reactive power (Q = I²X). Power factor correction aims to minimize reactive power.
Misconception: Higher Reactance Always Means Less Current
This is generally true for a given voltage, but the relationship is more complex. In resonant circuits, reactance can be canceled by capacitive reactance, creating maximum current flow. The total impedance, not just reactance, determines current flow.
Frequency Effects on Real Inductors
Real inductors have parasitic effects that become significant at high frequencies. Winding capacitance creates self-resonance, skin effect increases resistance, and core losses become important. These effects limit the useful frequency range of practical inductors.

Design Considerations:

  • Core Material: Ferrite for high frequencies, laminated steel for power applications
  • Winding Configuration: Minimize parasitic capacitance and resistance
  • Temperature Effects: Inductance and resistance change with temperature
  • Saturation: Magnetic cores saturate at high currents, reducing inductance

Mathematical Derivation and Examples

  • Reactance Formula Derivation
  • Impedance Calculations
  • Power Analysis
The mathematical foundation of inductive reactance comes from electromagnetic theory and circuit analysis. Understanding the derivation helps apply the concepts correctly in practical applications.
Derivation of XL = 2πfL
Starting with Faraday's law: V = -L(di/dt). For sinusoidal current i = Iₘsin(ωt), the voltage becomes V = -L(d/dt)[Iₘsin(ωt)] = -LωIₘcos(ωt) = LωIₘsin(ωt + 90°). The voltage amplitude is Vₘ = LωIₘ, so the reactance is XL = Vₘ/Iₘ = Lω = 2πfL.
Impedance in Series RL Circuits
In a series RL circuit, the total impedance is Z = √(R² + XL²), where R is the resistance and XL is the inductive reactance. The phase angle is θ = arctan(XL/R), and the current lags the voltage by this angle. The power factor is cos(θ) = R/Z.
Quality Factor Calculation
The quality factor Q = XL/R = ωL/R = 2πfL/R. It represents the ratio of stored energy to dissipated energy per cycle. High-Q inductors have low resistance relative to reactance, making them efficient for energy storage applications.
Power Calculations
In AC circuits with inductance, the apparent power S = VI, real power P = VIcos(θ), and reactive power Q = VIsin(θ). The power triangle relates these quantities: S² = P² + Q². Only real power is consumed; reactive power oscillates between source and load.

Practical Calculations:

  • Example 1: 100 mH inductor at 1 kHz: XL = 2π(1000)(0.1) = 628 Ω
  • Example 2: 10 μH inductor at 10 MHz: XL = 2π(10⁷)(10⁻⁵) = 628 Ω
  • Example 3: Power factor correction: To correct 0.8 lagging to 0.95, add capacitive reactance
  • Example 4: Resonant frequency: f = 1/(2π√(LC)) for LC resonance