RL Time Constant Calculator – Tau, Current Rise and Decay

RL Time Constant Calculator

Enter the inductance L, resistance R and supply voltage V of an RL circuit to find the time constant tau = L / R, the final steady current V / R, the current at any moment with I(t) = (V/R)(1 - e^-t/tau) for a rise or I0 e^-t/tau for a decay, plus the stored energy and the 5 tau settle time.

🎯Real RL Circuit Presets

⚡RL Circuit Inputs

Rise starts from zero; decay falls from I0 toward zero.

Coil inductance; pick the matching unit at right.

uH = 1e-6 H, mH = 1e-3 H, H = 1 H.

Total series resistance of the coil and circuit.

Applied DC voltage that drives the current rise.

Decay mode only: the current flowing before switch off.

Time after switching; used in time and decay modes.

us = 1e-6 s, ms = 1e-3 s, s = 1 s.

Rise mode: time to reach this current is reported.

Controls rounding on every result card.

Time constant tau 0 tau = L / R
Final steady current 0 A Ifinal = V / R
Current at time t 0 A from the RL curve
Energy and settle 0 J 5 tau settle time below

🔢Formula Snapshot

tauL / R
IfinV / R
I(t)(V/R)(1-e^-t/T)
5 tauSettle time

📊Tau Multiples and Percent of Final Current

Elapsed TimeRise: Percent of IfinalDecay: Percent RemainingState
0 tau0.0%100.0%Switch instant
0.5 tau39.3%60.7%Early
1 tau63.2%36.8%One constant
2 tau86.5%13.5%Rising fast
3 tau95.0%5.0%Near done
4 tau98.2%1.8%Almost full
5 tau99.3%0.7%Settled
7 tau99.9%0.1%Complete

🔌Common L and R to Time Constant

Inductance LResistance Rtau = L / R5 tau SettleTypical Use
47 uH1 ohm47 us235 usBuck converter
220 uH2 ohm110 us550 usBoost inductor
10 mH5 ohm2 ms10 msMotor winding
50 mH25 ohm2 ms10 msSolenoid coil
100 mH200 ohm0.5 ms2.5 msRelay coil
250 mH150 ohm1.67 ms8.33 msContactor coil
1 H50 ohm20 ms100 msFilter choke
5 mH0.5 ohm10 ms50 msIgnition primary

🧮RL Comparison Grid

Inductance LResistance RVoltage Vtau = L / RIfinal = V/R5 tau SettleEnergy 0.5 L I^2
47 uH1 ohm5 V47 us5 A235 us587.5 uJ
220 uH2 ohm12 V110 us6 A550 us3.96 mJ
10 mH5 ohm24 V2 ms4.8 A10 ms115.2 mJ
50 mH25 ohm24 V2 ms0.96 A10 ms23.04 mJ
100 mH200 ohm12 V0.5 ms0.06 A2.5 ms0.18 mJ
250 mH150 ohm24 V1.67 ms0.16 A8.33 ms3.2 mJ
1 H50 ohm48 V20 ms0.96 A100 ms460.8 mJ
5 mH0.5 ohm12 V10 ms24 A50 ms1.44 J

⚙Formula Breakdown

Time constant tau = L / RDivide inductance in henries by resistance in ohms. A 100 mH coil with 200 ohm gives tau = 0.1 / 200 = 0.0005 s, or 0.5 ms.
Final current Ifinal = V / ROnce the inductor is fully energized it looks like a wire, so the steady current is Ohm law. Here 12 V over 200 ohm gives 0.06 A.
Rise I(t) = (V/R)(1 - e^-t/tau)Current climbs toward Ifinal. At t = tau the factor 1 - e^-1 = 0.632, so I reaches 63.2 percent of the final value.
Decay I(t) = I0 e^-t/tauWhen the source is removed the current falls from its start value I0. At t = tau only e^-1 = 36.8 percent remains.
Settle time = 5 tauAfter five time constants the current is within 0.7 percent of its final state, treated as fully settled in practice.
Stored energy = 0.5 L Ifinal^2The magnetic field holds energy. With 0.1 H at 0.06 A this is 0.5 × 0.1 × 0.06^2 = 0.00018 J, or 0.18 mJ.

💡RL Design Tips

Current cannot change instantly: An inductor resists sudden change in current, so when a switch opens the coil tries to keep the same amps flowing. That forces the voltage to spike as high as needed, and V = L × di/dt can reach hundreds of volts across a small coil, enough to arc a switch or destroy a transistor.
Add a flyback diode: Place a diode across the coil, cathode to the positive supply, to give the collapsing current a safe loop when the drive turns off. The diode clamps the spike near 0.7 V and lets the stored energy decay through the coil resistance over roughly 5 tau instead of destroying the switching device.

Physics doesn’t like rapid changes in current so there’s some waiting around required for an RL circuit which we’ll call RC for now, since I’m lazy: you flip the switch and nothing happens. It takes a while. It crawls up a gentle exponential hill, which is determined by a simple ratio known as time constant (tau). This ratio governs how quickly a relay engage and also how long a solenoid will hold its spot once power is removed. Knowing about the delay help you avoid blasting transistors or other part.

Resistive: Because higher resistance limits the peak current, smaller tau. (Lower resistance allow more peak current into a coil, but it’s the inductance that resist the change.) Inductance means that the bigger the coil, the more magnetic field it hold, which makes it harder to change and results in a larger tau. When the magnetic field has stabilized, however, the inductor behave as though it’s just an ordinary wire. The current then obeys Ohm’s law, V/R… Settling down to whatever level the battery maintains after the inductor is removed.

Understanding RL Circuit Delays

For example, if you hook up a 200 ohm coil to a 12 volt supply, the final current will be 60 milliamps, and the calculator figures out algebra for you so it can display that ceiling value. Better yet, it displays how far from that ceiling you’re getting at every instant because the inductor follows a particular curve as it rises and falls. Specifically, when time reaches one tau, the rising current is 63 percent of its final value; and once the voltage drops below that point, the falling current is only 37 percent of original value. No matter what the component values might be, those two numbers will always hold true.

For example, take a standard relay coil that’s rated at 200 ohms of resistance and 100 millihenries of inductance. That works out to a time constant of half a millisecond. One tau later, current has climbed to about 38 milliamps. This might feel slow but it feels fast in terms of mechanical hardware. Five tau later, at 2.5 milliseconds, the current is within one percent of intended target value of 60 milliamps, so engineers define that five tau value as the settle time since any difference beyond that is negligible.

The tool does that calculation immediately for you, then lets you check whether you have sufficient time from your switching frequency to get the coil energized before shutting it down again. That’s why inductor timing is important (current doesn’t turn off immediately); there are also very large voltage spikes created as the coil attempts to maintain flow. This can damages semiconductor switches, or even cause arcing across contacts. A flyback diode safely conducts this energy away and reduces it (about 5x time constants). Because we know how fast the current turns off when the drive stops (see the table of references above), we can determine whether the system has sufficient time to safely bleed down, keeping components cool and running reliabley. You should of checked if parts stays cool too.

You can also see these trade-offs instantly with preset scenario. A small buck converter inductor takes only microseconds to run its course, while a big filter choke take milliseconds. You can do this all without doing math by hand. Then there are the inputs: You can switch between units (e.g., henries vs. Microhenries), and they’ll convert them all behind the scenes, so that you just plug in your components’ numbers, and it figures out the rest.

And then you have your answer: When does the current arrive? It shows how much energy is in the magnetic field at every moment. That is what matters when you want to size a snubber or understand heat load. Whether it’s a power supply with switching spikes or a moddern mechanical relay you’re trying to time correctly, get the numbers right and you’ll protect your hardware from the kind of stress you can’t see.

The rise/decay pace will be set by the time constant; it establishes the rhythm of the circuit. That makes the delay predictable but also real. Learn the pace and you learn how to design systems that respond fast while not burning out their component.

RL Time Constant Calculator – Tau, Current Rise and Decay