Capacitors, Inductors & AC Circuits

the time constant

When you connect a resistor to a capacitor (or inductor), things do not change instantly. They ease toward their final value along a smooth curve. The time constant tells you how fast: it is the natural settling pace of the circuit, like how long a warm cup takes to cool toward room temperature.

For a resistor R charging a capacitor C, the time constant is tau = R times C. In tau seconds the voltage covers about 63 percent of the remaining gap to its final value; after about 5 tau it is within 1 percent, effectively done. Example: R = 10 kilohm and C = 10 uF give tau = 10000 times 0.00001 = 0.1 second, so the capacitor is essentially fully charged in about half a second. For an inductor-resistor pair the time constant is tau = L/R instead.

The approach is exponential: the curve is steep at first and flattens as it nears the target, never quite a straight line. Time constants set switch-debounce delays, the response of RC filters, and how fast a decoupling capacitor recharges. Caveat: fully charged is an approximation. Mathematically it only reaches the target at infinity; in practice 5 tau is close enough.

R = 1 kilohm, C = 100 uF give tau = 0.1 s. Starting from 0 V toward 5 V, after 0.1 s the capacitor reaches about 3.16 V (63 percent), and after 0.5 s about 4.97 V.

One time constant covers 63 percent of the gap.

It is tau = RC for an RC circuit but tau = L/R for an RL circuit. The inductor's resistance divides rather than multiplies, and mixing the two formulas is a common slip.

Also called
tauRC time constant時常數