How this calculator works
- Step 1Time constantτ = R × CSets how fast everything happens.
- Step 2ChargingVs (1 − e^(−t/τ))Fast at first, then slowing.
- Step 3DischargingVs e^(−t/τ)The mirror image.
When a capacitor charges through a resistor, the current starts high and falls as the capacitor fills. The voltage rises quickly at first and then levels off.
The time constant τ = R × C sets the pace. After one τ the capacitor is 63.2% of the way there; after five it is 99.3%.
Worked example: 1 kΩ and 1,000 µF on 9 V
- τ
R × C- V(t)
Vs × (1 − e^(−t/τ))
- Time constant1,000 Ω × 0.001 F1.0000 s
- Share complete1 − e⁻¹63.21%
- Capacitor voltage9 × 63.21%5.6891 V
Read the result
Discharging is the mirror image: from 9 V the same capacitor falls to 3.3109 V after 1 s.
- 4.7 kΩ, 220 µF1.0340 sOn 12 V it reaches 10.2656 V after 2 s.
- Full charge5.1700 sFive time constants: 99.3% of the supply.
Assumptions and limits
- Ideal partsNo leakage or internal resistance in the source.
- Steady supplyThe supply voltage does not sag.
- ToleranceReal capacitors are often ±10–20%.
- No inductanceRL and RLC circuits behave differently.
Related electrical tools
An RC circuit charges along an exponential curve set by resistance and capacitance.
To combine resistors first, use the series and parallel resistor calculator. The Ohm’s law calculator relates voltage and current, and the half-life calculator uses the same exponential decay.
Common mistakes
Mistake: Using µF as farads in τ = RC.
Instead: Multiply µF by 10⁻⁶; this tool does it for you.
Mistake: Expecting a full charge after one τ.
Instead: One τ is 63.2%; allow about 5 τ.
Checking the method
A separate script steps the circuit equation forward numerically, without the exponential formula, and matches every golden voltage.
Read how we test our calculators, or browse more maths calculators.