RC Time Constant Calculator

Enter the resistor, the capacitor and the voltage, and choose charging or discharging. You get the time constant τ, the voltage after a time you choose, the time to reach a level, the low-pass cutoff frequency and a chart of the curve.

Free Runs in your browser Checked Tuesday, November 10, 2026

Circuit

Charging: the capacitor fills from a supply. Discharging: it empties through the resistor.

The voltage the capacitor charges to, or had when discharging started, in volts.

The series resistor. Type 10k for 10 kΩ or 4k7 for 4.7 kΩ.

The capacitance. Type 100µ for 100 µF or 100n for 100 nF.

The moment at which you want the voltage, counted from the start of charging or discharging.

Charging: the percentage of the supply voltage to reach. Discharging: the percentage of the starting voltage left.

Result

Time constant τ = R × C — The time for the voltage to change by about 63 % of its total change.
Low-pass cutoff frequency — The frequency where an RC low-pass filter passes half the power, 1 ÷ (2π × R × C).
Voltage at time t —
Time to reach the level —

Voltage from 0 to 5τ

Working, step by step

This tool runs in your browser. What you enter is not sent to us.

How to use it

  1. Choose Circuit: Charging or Discharging.
  2. Type the Supply voltage (or starting voltage), the Resistor R and the Capacitor C.
  3. Type the Time t (seconds) you want to check and the Level to reach (%).
  4. Read Time constant τ and Voltage at time t, then look at the chart to see the curve from 0 to 5τ.

The formulas

A resistor and a capacitor in series change their voltage exponentially. The product R × C is the time constant τ: after one τ a charging capacitor has reached 63.2 % of its final voltage, and a discharging one has fallen to 36.8 % of its start.

τ = R × C

Charging:    V(t) = Vs × (1 − e^(−t ÷ τ))
Discharging: V(t) = V0 × e^(−t ÷ τ)

Time to reach p %:
Charging:    t = −τ × ln(1 − p)
Discharging: t = −τ × ln(p)

Low-pass cutoff: f = 1 ÷ (2π × R × C)
  • After 5τ the capacitor is more than 99.3 % charged, and less than 0.7 % of the starting voltage remains. Most practical timing uses 5τ as the 'done' point.
  • The cutoff frequency is the point where a low-pass RC filter passes half the power, which is 0.707 of the voltage.
  • The chart covers 0 to 5τ in 25 equal steps.

What this calculator does not cover

  • The source resistance and the leakage of a real capacitor, which lengthen the charging time.
  • Circuits with more than one resistor or capacitor, and RC filters with a load across the output.
  • Pulses that start before the capacitor is empty: the starting voltage then depends on the earlier cycle.

Worked example: 10 kΩ and 100 µF charged from 5 V

τ = 10 kΩ × 100 µF = 1 s. The cutoff of a low-pass made of the same parts is 1 ÷ (2π × 1 s) = 159.2 mHz.

After 2 s the capacitor voltage is 5 V × (1 − e^(−2)) = 4.323 V.

The voltage reaches 63.2 % of the supply, 3.16 V, after one time constant. The exact time to reach 63.2 % is −1 s × ln(1 − 0.632) = 999.7 ms, because 0.368 is just above e⁻¹.

Frequently asked questions

What does the time constant tell me?

It is the time for a charging capacitor to reach about 63 % of its final voltage, or a discharging one to fall to about 37 % of its start. Five time constants is the time for it to be practically full or empty.

Why does the chart run from 0 to 5τ?

After 5τ a charging capacitor is more than 99.3 % charged and a discharging one has lost more than 99.3 % of its voltage, so the curve has effectively finished.

How is the cutoff frequency of a filter found?

Use f = 1 ÷ (2π × R × C) with the resistor and capacitor of the filter. A signal above this frequency is weakened, and one below it passes.

Can I enter the capacitance in nanofarads?

Yes. Type 100n for 100 nF or 2µ2 for 2.2 µF. The calculator converts the prefixes before the calculation, so τ comes out in seconds.

What is the difference between charging and discharging?

Charging starts from zero and approaches the supply voltage; discharging starts from the stored voltage and approaches zero. Both follow the same time constant, so the same R and C give the same speed.

Sources

Figures and text last checked on Tuesday, November 10, 2026.

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