0.0001
s
1,591.5494
Hz
0.0005
s
100
Ω
0.0001
s
1,591.5494
Hz
0.0005
s
100
Ω
The RL circuit calculator helps engineers and students analyze resistor-inductor circuits, a fundamental class of circuits found throughout power electronics, RF engineering, motor drives, and signal conditioning systems. An RL circuit combines a resistor (R) with an inductor (L), and its behavior is governed by the relationship between energy storage in the magnetic field and dissipation in the resistance.
The time constant of an RL circuit, τ = L/R, defines how quickly current builds up in the circuit after a voltage is applied. Unlike an RC circuit where the time constant increases with larger capacitance, in an RL circuit a larger inductance slows the current rise while a larger resistance speeds it up. After one time constant, current reaches 63.2% of its steady-state value (V/R). After five time constants, current is at 99.3% — the circuit is considered to have reached steady state.
RL circuits are ubiquitous in power electronics. Every transformer, motor winding, relay coil, and solenoid is an RL circuit. Understanding the time constant is crucial for calculating inductive kick (flyback voltage), designing gate driver circuits for MOSFETs and IGBTs, and protecting circuits from transient overvoltages. Snubber circuits and freewheeling diodes are designed based on the RL time constant to safely dissipate stored magnetic energy.
As filters, RL circuits form high-pass filters when the output is taken across the inductor, and low-pass filters when taken across the resistor. The cutoff frequency fc = R/(2πL) marks the -3 dB point where inductive reactance equals resistance (XL = R). Above this frequency for a high-pass RL filter, the inductor's impedance dominates; below it, the resistor dominates.
Inductive reactance XL = 2πfL increases linearly with frequency, making inductors increasingly effective at blocking high-frequency signals. This property is exploited in EMI filters, chokes in power supplies, and RF bias networks where inductors present high impedance to RF signals while passing DC.
This calculator provides the time constant, cutoff frequency, settle time (5τ), and inductive reactance at the cutoff frequency. Input resistance in ohms and inductance in millihenries (mH) for most practical circuit design work.
For power electronics applications, always check the inductor's saturation current rating. An inductor that saturates loses its inductance, causing current to rise much faster than the RL time constant predicts, potentially damaging MOSFETs and other switching devices.
Time constant: τ = L/R, with L in henries and R in ohms. Inductance is entered in millihenries and converted by multiplying by 10⁻³. Cutoff frequency: fc = R/(2πL), the frequency where inductive reactance XL = R. Settle time: 5τ, when current reaches 99.3% of steady state. At the cutoff frequency, XL = R by definition, so the reactance output always equals R.
A large time constant (high L, low R) means current rises slowly — important in power inductors to limit inrush current. A small time constant (low L, high R) gives fast current response — needed in switching regulators with fast transient response. The cutoff frequency determines the filter bandwidth: signals below fc pass through a low-pass RL filter with less than 3 dB attenuation.
Inputs
Results
A motor winding with R = 5 Ω and L = 50 mH has τ = 10 ms. Current ramps to steady state in ~50 ms after applying voltage.
Inputs
Results
L = 1000 mH and R = 50 Ω gives fc ≈ 8 Hz — this choke passes audio frequencies but blocks DC switching transients effectively.
The RL time constant τ = L/R (in seconds) is the time for current to rise to 63.2% of its final steady-state value V/R after a step voltage is applied.
In an RC circuit, voltage across the capacitor changes gradually (τ = RC). In an RL circuit, current through the inductor changes gradually (τ = L/R). Both circuits exhibit exponential transient behavior.
Inductive reactance XL = 2πfL is the opposition an inductor offers to AC current. Unlike resistance, it increases with frequency. At the cutoff frequency, XL equals R.
An inductor stores energy ½LI² in its magnetic field. When current is interrupted suddenly, the inductor maintains current by generating a large voltage spike (V = L × dI/dt). Freewheeling diodes and snubbers are used to dissipate this energy safely.
The cutoff frequency fc = R/(2πL) is the -3 dB frequency where inductive reactance equals resistance. Above this frequency, an RL low-pass filter attenuates the signal at 20 dB per decade.
Yes — this calculator accepts inductance in millihenries and converts internally. For microhenries (µH), divide by 1000 before entering. For henries, multiply by 1000.
The quality factor Q = XL/R = 2πfL/R. It indicates the energy storage-to-dissipation ratio. Higher Q means less resistive loss and sharper filter response. This calculator does not directly compute Q, but you can derive it from XL and R at any given frequency.
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