⚡ RC Circuit Calculator
Calculate the time constant and maximum charge of a Resistor-Capacitor circuit.
Inputs
Note: 1 µF = 0.000001 F
Results
Capacitor Charging Curve
Calculator Description
An RC circuit is the simplest first-order dynamic circuit, made of a resistor (R) and a capacitor (C). When the source is switched on or off, the voltage and charge do not change instantly but transition exponentially — the foundation of filters, delays and integrator/differentiator circuits.
What this calculator finds
It computes the circuit time constant (τ), the capacitor’s maximum charge (Q), and the capacitor voltage V_c(t) at time t. Both the charging and discharging curves are described by the time constant.
Why it matters
- Designing RC low-pass/high-pass filter cutoff frequencies (1/2πRC)
- Reset delays, debouncing and timing in digital circuits
- Estimating settling time of sample-and-hold ADC inputs
Formula
RC Circuit Formulas
The time constant τ is the product of resistance and capacitance and is the time to reach about 63.2% of the final value. The charging voltage follows an exponential curve asymptoting to the source voltage V.
- τ — Time constant [seconds, s]
- R — Resistance [ohms, Ω]
- C — Capacitance [farads, F]
- V — Source voltage [volts, V]
- t — Elapsed time [seconds, s]
- Q — Capacitor charge [coulombs, C]
How the formula works
- A larger R or C gives a larger τ, so the capacitor charges more slowly.
- Each τ closes ~63.2% of the remaining gap; after 5τ the capacitor is considered ~99.3% charged.
- During discharge V_c(t) = V₀·e^(−t/τ), an exponential decay.
Cutoff frequency
The −3 dB cutoff of an RC filter is f_c = 1/(2πRC) = 1/(2πτ). A larger τ shifts the passband to lower frequencies.
Worked example
For R = 10 kΩ, C = 100 µF and V = 5 V, τ = 10×10³ × 100×10⁻⁶ = 1 s. Maximum charge Q = C·V = 100×10⁻⁶ × 5 = 500 µC. At t = 1 s, V_c = 5 × (1 − e⁻¹) ≈ 3.16 V — about 63.2% of the final value.
Useful Tips
Practical tips
- Pick R and C from the required delay/settling time, then consider leakage current and load capacitance.
- For input debouncing, make τ long enough relative to the bounce duration.
- A large capacitor ESR makes the charge curve deviate from the ideal exponential.
Limitations & cautions
- Assumes ideal R and C, ignoring leakage, ESR and inductance.
- Connecting a capacitor directly to a source causes a large inrush current — consider series resistance.
- At high frequency, wiring inductance and parasitics dominate and the first-order model becomes inaccurate.