Capacitance and Uses of Capacitors
Capacitance
Capacitance (symbol C) is a measure of a capacitor's ability to store charge. A large capacitance means that more charge can be stored. Capacitance is measured in farads, symbol F. However 1F is very large, so prefixes (multipliers) are used to show the smaller values:- µ (micro) means 10-6 (millionth), so 1000000µF = 1F
- n (nano) means 10-9 (thousand-millionth), so 1000nF = 1µF
- p (pico) means 10-12 (million-millionth), so 1000pF = 1nF
Charge and Energy Stored
The amount of charge (symbol Q) stored by a capacitor is given by:Charge, Q = C × V | where: | Q = charge in coulombs (C) C = capacitance in farads (F) V = voltage in volts (V) |
Energy, E = ½QV = ½CV² where E = energy in joules (J). |
Capacitive Reactance Xc
Capacitive reactance (symbol Xc) is a measure of a capacitor's opposition to AC (alternating current). Like resistance it is measured in ohms,
Capacitive reactance, Xc = | 1 | where: | Xc = reactance in ohms (![]() f = frequency in hertz (Hz) C = capacitance in farads (F) |
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For example a 1µF capacitor has a reactance of 3.2k


Note: the symbol Xc is used to distinguish capacitative reactance from inductive reactance XL which is a property of inductors. The distinction is important because XL increases with frequency (the opposite of Xc) and if both XL and Xc are present in a circuit the combined reactance (X) is the difference between them. For further information please see the page on Impedance.

Capacitors in Series and Parallel
Combined capacitance (C) of capacitors connected in series: |
1 | = | 1 | + | 1 | + | 1 | + ... |
C | C1 | C2 | C3 |
Combined capacitance (C) of capacitors connected in parallel: |
C = C1 + C2 + C3 + ... |
Note that these equations are the opposite way round for resistors in series and parallel.
Charging a capacitor

At first Vc = 0V so the initial current, Io = Vs / R
Vc increases as soon as charge (Q) starts to build up (Vc = Q/C), this reduces the voltage across the resistor and therefore reduces the charging current. This means that the rate of charging becomes progressively slower.
time constant = R × C | where: | time constant is in seconds (s)
R = resistance in ohms ( ![]() C = capacitance in farads (F) |
If R = 47k


If R = 33k


A large time constant means the capacitor charges slowly. Note that the time constant is a property of the circuit containing the capacitance and resistance, it is not a property of a capacitor alone.
Graphs showing the current and voltage for a capacitor charging time constant = RC |
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Discharging a capacitor
Graphs showing the current and voltage for a capacitor discharging time constant = RC |
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Initial current, Io = Vo / R.
Note that the current graphs are the same shape for both charging and discharging a capacitor. This type of graph is an example of exponential decay.
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After 5 time constants (5RC) the voltage across the capacitor is almost zero and we can reasonably say that the capacitor is fully discharged, although really discharging continues for ever (or until the circuit is changed).
Uses of Capacitors
Capacitors are used for several purposes:- Timing - for example with a 555 timer IC controlling the charging and discharging.
- Smoothing - for example in a power supply.
- Coupling - for example between stages of an audio system and to connect a loudspeaker.
- Filtering - for example in the tone control of an audio system.
- Tuning - for example in a radio system.
- Storing energy - for example in a camera flash circuit.
Capacitor Coupling (CR-coupling)

For successful capacitor coupling in an audio system the signals must pass through with little or no distortion. This is achieved if the time constant (RC) is larger than the time period (T) of the lowest frequency audio signals required (typically 20Hz, T = 50ms).
Output when RC >> T
When the time constant is much larger than the time period of the input signal the capacitor does not have sufficient time to significantly charge or discharge, so the signal passes through with negligible distortion.
Output when RC = T
When the time constant is equal to the time period you can see that the capacitor has time to partly charge and discharge before the signal changes. As a result there is significant distortion of the signal as it passes through the CR-coupling. Notice how the sudden changes of the input signal pass straight through the capacitor to the output.
Output when RC << T
When the time constant is much smaller than the time period the capacitor has time to fully charge or discharge after each sudden change in the input signal. Effectively only the sudden changes pass through to the output and they appear as 'spikes', alternately positive and negative. This can be useful in a system which must detect when a signal changes suddenly, but must ignore slow changes.
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