Capacitor Calculator
Free capacitor calculator — solve charge, capacitance or voltage from Q = CV, plus the RC time constant, with an animated charging diagram.
Free capacitor calculator — solve charge, capacitance or voltage from Q = CV, plus the RC time constant, with an animated charging diagram.
Q = C × V, with charge in coulombs, capacitance in farads and voltage in volts. Add a series resistor and the charging follows an exponential curve with a time constant, written τ (the Greek letter tau), equal to resistance × capacitance: 63% of the way there after one τ, and effectively complete after five.
A reservoir capacitor fills the gaps between rectifier peaks, turning a lumpy waveform into something a circuit can actually run on.
A battery charges the capacitor slowly over a second or two, and the capacitor dumps it all in a millisecond. Batteries cannot do that.
An RC pair sets the delay in a 555 timer, a blinking light or a debounce circuit. Pick the two values and you pick the timing.
Capacitors pass changing signals and block steady DC, which is how one stage of an amplifier feeds the next without dragging its bias along.
A large capacitor near the amplifier supplies the sudden current a bass note demands, so the headlights stop dimming with the beat.
A charged capacitor keeps a clock or a settings chip powered through a short interruption, which is why some devices keep the time through a power cut.
It stores energy in an electric field between two conducting plates separated by an insulator. Charge builds on the plates until the voltage across them matches whatever is driving them. Unlike a battery, which stores energy chemically and releases it slowly at a fairly steady voltage, a capacitor stores far less energy but can deliver and absorb it almost instantly. That speed is what makes it useful for smoothing supplies, filtering signals and buffering sudden current demands.
Q equals C times V — charge in coulombs is capacitance in farads multiplied by voltage. The farad is an enormous unit, so real components are marked in microfarads, nanofarads and picofarads. A 100 µF capacitor at 12 V holds 100 × 10⁻⁶ × 12 = 1.2 × 10⁻³ coulombs, or 1,200 microcoulombs. Keeping the powers of ten straight is where most errors in this calculation happen.
When a capacitor charges through a resistor the voltage rises exponentially rather than linearly, and the time constant τ = R × C sets the pace. After one time constant the capacitor has reached about 63% of the supply voltage, after three about 95%, and after five roughly 99% — treated as fully charged for practical purposes. A 100 µF capacitor through a 10 kΩ resistor gives τ = 1 second, so it is effectively charged after five.
Because one farad means storing one coulomb of charge per volt, and a coulomb is an enormous quantity of charge — about 6.24 × 10¹⁸ electrons. Ordinary capacitors are in the microfarad range or below, and even a supercapacitor rated at several farads is physically substantial. The unit was defined from the underlying physics rather than from anything convenient to build, which is why practically every real component is marked with a prefix.
A battery stores energy chemically, holds a roughly constant voltage as it discharges, and packs far more energy per unit volume. A capacitor stores energy physically in a field, its voltage falls steadily as it discharges, and it holds perhaps a thousandth as much energy for the same size. What a capacitor offers instead is power: it can dump its energy in microseconds and be recharged endlessly without wearing out, where a battery would be damaged by either.