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RL Circuit Time Constant Calculator

Calculate the time constant and current charging curve for a resistor-inductor (RL) circuit.

Result

Time Constant (τ)
0.5 ms
Current at Given Time
86.5% of max

Formula: τ = L/R. Current in an RL circuit rises according to I(t) = Iₘₐₓ(1 - e^(-t/τ)), reaching about 63.2% of its maximum value after one time constant, similar in shape to an RC circuit's charging curve but governed by inductance and resistance instead of capacitance and resistance.

About the RL Time Constant

This calculator finds the time constant of a resistor-inductor (RL) circuit and shows what fraction of maximum current has built up by a chosen moment after the circuit closes. It is aimed at anyone working with inductive loads, such as relay coils, motor windings, or transformer primaries, who needs to know how quickly current ramps up rather than assuming it turns on instantly. Because inductors resist sudden changes in current, this ramp-up time matters for switching circuit design, timing relays, and understanding transient behavior in power electronics.

How It Works

You enter the inductance in millihenries, the resistance in ohms, and how much time has passed since the circuit closed, in milliseconds. The calculator converts inductance to henries and computes the time constant tau = L/R (with resistance floored at 0.001 ohm to avoid dividing by zero), then reports how many milliseconds one time constant takes. It also plugs your elapsed time into the exponential charging equation to show what percentage of maximum current the circuit has reached at that instant.

tau = L / R (inductance in henries, resistance in ohms); current at time t: I(t) = I_max * (1 - e^(-t/tau))

Formula & Methodology

To work this by hand, convert inductance to henries by dividing millihenries by 1000, then divide by resistance in ohms to get tau in seconds, and multiply by 1000 for tau in milliseconds. To find the percent of maximum current at a given elapsed time, convert that time to seconds, divide it by tau, negate the result, raise e to that power, subtract from 1, and multiply by 100.

Examples

Relay coil energizing

With a 50 mH coil and 100 ohm resistance, tau works out to 0.5 ms. One millisecond after the circuit closes, two time constants, the current has reached about 86.5 percent of its final value.

One time constant checkpoint

A 200 mH inductor in series with a 50 ohm resistor gives tau = 4 ms. At exactly 4 ms elapsed, the current sits at 63.2 percent of maximum, the universal one-time-constant benchmark for exponential charging.

Advantages

  • Converts millihenries and milliseconds automatically so you don't have to manually shift decimal places between henries and seconds.
  • Reports both the time constant and the instantaneous percent of maximum current in one calculation, saving a second manual step with the exponential formula.
  • Useful for sanity-checking datasheet values or lab measurements against the theoretical RL charging curve.

Common Mistakes

  • Entering inductance in henries instead of millihenries, or vice versa, which throws the time constant off by a factor of 1000.
  • Forgetting that the elapsed time field is measured from when the circuit closes, not from an arbitrary starting point, leading to a misread percentage.
  • Assuming current jumps to its full value instantly, when an inductor guarantees a gradual, exponential rise governed entirely by L and R.

Edge Cases to Watch For

  • Resistance is floored at 0.001 ohm internally, so entering zero or a negative resistance won't cause a divide-by-zero error, but it produces an unrealistically fast time constant that doesn't reflect any real circuit.
  • The calculator assumes an ideal inductor with no internal resistance or parasitic capacitance; real inductors have winding resistance that changes the effective time constant.
  • At elapsed times many multiples of tau, roughly five tau or more, the reported percent of maximum current rounds to 100 percent since the exponential term becomes negligible.

Common Use Cases

  • Electronics students verifying textbook RL transient problems against a working formula.
  • Hobbyists and technicians sizing relay or solenoid drive circuits where switching speed matters.
  • Engineers checking how quickly an inductive load reaches steady-state current after a switch closes.
Written & fact-checked by the Calculateus TeamLast updated August 5, 2026How we verify our formulas

Frequently asked questions

How is an RL circuit's behavior different from an RC circuit's?

Both follow the same exponential charging/discharging shape, but an inductor opposes changes in current (storing energy in a magnetic field) while a capacitor opposes changes in voltage (storing energy in an electric field) - this means current rises gradually in an RL circuit when voltage is first applied, the opposite of a capacitor, which initially allows current to flow freely before charging up and blocking further current.

Conclusion

The RL time constant is a fixed property of the circuit's inductance and resistance alone, independent of the supply voltage. Once you know tau, this calculator lets you read off the current at any moment during the charging transient without solving the differential equation by hand.