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RC Time Constant Calculator
A capacitor charges through a resistor along a curve, not a straight line. The time constant τ = R × C is how long it takes to reach 63.2 % of the final voltage, and after about 5 τ it is practically full (99.3 %).
Result
Charging from empty
- After 1 τ (1 s)
- 63.2 % · 3.161 V
- After 2 τ (2 s)
- 86.5 % · 4.323 V
- After 3 τ (3 s)
- 95.0 % · 4.751 V
- After 4 τ (4 s)
- 98.2 % · 4.908 V
- After 5 τ (5 s)
- 99.3 % · 4.966 V
Your questions
- Time to reach 50 %while charging from empty
- 693.1 ms
- Charging, after 1 s
- 3.161 V (63.2 %)
- Discharging, after 1 sstarting full
- 1.839 V (36.8 %)
After about 5 τ a capacitor is practically full (99.3 %). It never reaches exactly 100 %.
The formula
What each letter means
- Time constant τ (tau) (s · second) : How long an RC or RL circuit takes to get 63 % of the way to its final value. After 5τ it is basically done.
- Resistance (Ω · ohm) : How strongly something opposes current.
- Capacitance (F · farad) : How much charge a capacitor stores per volt.
- Voltage across the capacitor (V · volt)
- Supply voltage (V · volt) : The source or supply voltage.
- Euler’s number e ≈ 2.718 (no unit) : A fixed number used for anything that grows or decays smoothly, such as a capacitor charging. Not a variable.
- Time (s · second) : Time since something started.
- Charge level wanted (% · percent) : How full you want the capacitor, as a percent of its final voltage. It must be below 100 %, because it only ever gets closer.
How it works
While a capacitor is nearly empty, a lot of current flows into it and it charges quickly. As it fills, the voltage across the resistor shrinks, the current drops and the charging slows down. Every time constant τ closes 63.2 % of the gap that is left, which is where the table of 63.2 %, 86.5 %, 95.0 %, 98.2 % and 99.3 % comes from: each one is 1 − e^−n for n = 1 to 5.
Discharging is the mirror image: the voltage falls to 36.8 % after 1 τ, 13.5 % after 2 τ, and so on. The supply voltage does not change τ. A bigger resistor or a bigger capacitor makes everything slower in proportion.
Worked example
- R = 10 kΩ and C = 100 µF. The time constant is τ = R × C = 1 s.
- After 1 τ the capacitor is 63.2 % charged, and after 5 τ it is 99.3 % charged. With a 5 V supply that is 3.161 V and 4.966 V.
- To reach 50 %: t = −τ × ln(1 − 0.5) = 693.1 ms (that is τ × ln 2).
- After 1 s a capacitor charging from empty is at 3.161 V. One that started full and is discharging is at 1.839 V. They add up to the 5 V supply.
Common questions
Why can a capacitor never reach 100 %?
Each time constant only closes 63.2 % of the distance that remains, so there is always a small gap left. In practice the gap becomes too small to measure after a few τ, which is why 100 % is not a valid answer in the time box.
Why do people use 5 τ?
After 5 τ the capacitor has reached 99.3 % of its final voltage. That is close enough to “full” for most circuits, such as a power-on reset delay or a button debounce, so 5 τ is the usual waiting time.
Does the supply voltage change the time constant?
No. τ depends only on R and C. A higher supply makes the capacitor end up at a higher voltage, but it still takes the same time to reach the same percentage.
Try it live
- Try it live in lesson 2.2: RC Time Constant: Capacitor Charging Explained
- Try it live in lesson 4.1: Pull-Up Resistors & Button Debounce Explained
- Component guide: Capacitor
- Component guide: Resistor