⚡ Spark Academy53 lessons

Capacitors & the RC Time Constant

A component that stores charge and, paired with a resistor, tells time. This lesson powers your final build's heartbeat.

lesson 3 of 4 in this unit

Builds on: 0.1 Electric Charge & the Atom0.2 Voltage: Energy per Charge1.2 Ohm's Law

A bucket for charge

A capacitor is two conducting plates separated by an insulator. Push current in and charge piles onto one plate while the other is drained, building a voltage across the gap — Lesson 0.2’s charged plates, now as a component. How much charge it holds per volt is its capacitance:

Q = C × Vfarads = coulombs per volt · practical parts: pF, nF, µF

One farad is enormous; real circuits use microfarads and smaller. Two habits to build now: electrolytic capacitors (the little cans, µF range) are polarized — the striped leg must go to the lower voltage or they can fail dramatically. And big charged capacitors keep their charge after power-off; treat them with respect.

Charging through a resistor: the exponential

Feed a capacitor through a resistor and it can’t fill instantly: the fuller it gets, the smaller the remaining voltage across R, the smaller the current refilling it. The result is the most famous curve in electronics — fast at first, ever slower, never quite arriving:

V(t) = V_s (1 − e^(−t/RC))  ·  τ = R × Cτ in seconds when R in ohms, C in farads
elapsedcharged to
63%
86%
95%
≈ 99% — call it done

The shape is universal. 1 kΩ × 100 µF gives τ = 0.1 s; 10 kΩ × 100 µF gives 1 s — same curve, different clock speed. Discharging mirrors it: down to 37% after one τ.

What capacitors are for

  • Timing: charge to a threshold, trigger something, repeat — this is precisely how your 555 blinker will tick.
  • Smoothing: a capacitor across a supply is a reservoir that fills the dips — every power supply has them.
  • Blocking DC: once charged, no steady current flows through — but wiggles pass. Audio circuits couple stages this way.
  • Energy storage: camera flashes dump a capacitor in a millisecond — power no small battery could deliver.

⚡ Lab — The Universal Curve

An RC circuit on a live oscilloscope. The time axis re-scales to whatever τ you dial in.

  • Watch one full charge. Confirm it crosses the 63% line after one grid division (1τ).
  • Flip to discharge mid-curve — the capacitor doesn’t care, it just heads for its new target.
  • Change R and C wildly: the axis labels change, the shape never does.
1 kΩ
100 µF
τ = R × C
100 ms
The universal curve
change R or C: the labels change, the shape never does

Check your understanding

Q1. τ for R = 1 kΩ and C = 100 µF is…

Q2. After one time constant of charging, the capacitor has reached about…

Q3. A fully charged capacitor in a DC circuit carries how much steady current?

Q4. Your timer runs too fast. Using τ = RC, you could slow it by…