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Reminder sheet

Capacitors

Bastaya

A capacitor stores charges and therefore energy; it charges and discharges with a time constant τ = R·C. Remember 63 % at τ and "done" at 5τ.

A capacitor is made of two conducting plates separated by an insulator. At a voltage U it stores a charge Q = C·U; C is its capacitance, in farads (in practice µF, nF, pF). It stores the energy W = ½ C U².

In parallel capacitances add up; in series their inverses add up. Charged through a resistor, it reaches 63 % of its final voltage after τ = R·C and ≈ 100 % after 5τ; in steady DC it passes no current.

Formulas

CapacitanceQ = C · U
QuantitySymbolUnit
ChargeQC
CapacitanceCF
VoltageUV
Stored energyW = ½ · C ·
QuantitySymbolUnit
EnergyWJ
Combinationsparallèle : Céq = C₁ + C₂
série : 1Céq = 1C₁ + 1C₂
QuantitySymbolUnit
Equivalent capacitanceCéqF
RC time constantτ = R · C
QuantitySymbolUnit
Time constantτs
ResistanceRΩ
CapacitanceCF

3-digit marking: two digits then number of zeros, in pF (104 = 100 000 pF = 100 nF).

Worked example

A 100 µF capacitor is charged at 12 V. What charge and energy does it store? It is charged through R = 10 kΩ: time constant and charging time? Two such capacitors in series: equivalent capacitance?

Q = C · U = 100 × 10⁻⁶ × 12 = 1.2 × 10⁻³ C = 1.2 mC.

W = ½ · C · U² = 0.5 × 100 × 10⁻⁶ × 144 = 7.2 mJ.

τ = R · C = 10⁴ × 10⁻⁴ = 1 s: 63 % of 12 V (7.6 V) after 1 s, full charge (99 %) after 5τ = 5 s.

In series: 1/Ceq = 1/100 + 1/100, Ceq = 50 µF.

Common mistakes

  • Forgetting the 10⁻⁶ factor of microfarads: 100 µF = 10⁻⁴ F.
  • Applying the resistor rules: for capacitors it is the other way round: capacitances add in parallel, reciprocals add in series.
  • Believing that a charged capacitor lets a direct current through: once charged, the branch is an open circuit.

IEC symbols

Capacitor

Illustration

τ63 %U

Capacitor charging through R: 63 % of the final voltage after τ = RC.

Frequently asked questions

Why 63 % after one time constant?
The voltage rises as u = U (1 − e^(−t/τ)): at t = τ, 1 − 1/e ≈ 0.63. At 3τ it is 95 %, at 5τ more than 99 %: the charge is considered complete.
What is a capacitor for in direct current?
To store energy and release it (flash, buffer), to smooth a rectified voltage, to time a delay (RC circuit). In steady state it draws nothing.

17 exercises in this topic

Simulated time00:00:00
Q = I·t-
W = P·t-

Workbench

Circuit diagram CEI 60617

How does it work?

The perfboard: each big hole is a circuit node. You push a single leg of a component (resistor, lamp...) into it. The 4 small holes around it are connected to it: that is where chips and leads plug in.

  1. Drag a component onto the board: it snaps onto the grid. R rotates it.
  2. To join neighbouring big holes, click Jumper chip in the palette (or C) then drag on the board: a line of chips is laid at once. Bridged holes become a single node.
  3. For long links and for the power supply (placed next to the board), drag a lead from one big hole to another (or to a terminal).
  4. As soon as a loop is closed, the circuit is solved in real time (Ohm + Kirchhoff) and the diagram follows.
  5. Zoom with the wheel (or + / , two-finger pinch); drag the background to pan, 0 fits the board. The + buttons around the board add a row or a column.

Del delete · R rotate · C chip brush · Esc cancel · wheel zoom · drag the background to pan

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