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Electronic Parts

Discrete Components

Capacitors

Basics

A capacitor stores separated electric charge. The amount of charge stored for a given voltage is its capacitance:

C = Q / V
Units
UnitValueExample
farad (F)1 FLarge for ordinary electronics.
microfarad (µF)10−6 FPower filtering, audio coupling.
nanofarad (nF)10−9 FFilters and timing.
picofarad (pF)10−12 FRF and small-signal circuits.
0.1 µF = 100 nF = 100,000 pF
Voltage rating

The voltage rating is not the voltage a capacitor automatically produces; it is a limit on the voltage that may be applied. Designers normally leave margin for supply tolerance, ripple, transients, temperature, aging, and the rules of the particular capacitor technology.

Capacitors in parallel

Parallel capacitors have the same voltage across them and their capacitances add:

Ctotal = C1 + C2 + C3 + ...
10 µF and 22 µF in parallel give approximately 32 µF.
Capacitors in series

Series capacitors carry equal charge. Their total capacitance is lower than the smallest individual capacitance:

1 / Ctotal = 1 / C1 + 1 / C2 + ...

For two capacitors:

Ctotal = (C1 × C2) / (C1 + C2)
Series connection does not guarantee that voltage will divide equally. Leakage differences can produce unequal DC voltages, so high-voltage series stacks may require balancing resistors or active balancing.
Charging through a resistor

A resistor in series with a capacitor limits charging current. The product R × C is the time constant:

τ = R C

After one time constant, an initially discharged ideal capacitor charged from a fixed source has reached about 63% of its final voltage. After about five time constants it is very close to the final value.

10 kΩ and 100 µF:
τ = 10,000 × 0.0001 = 1 second
DC and AC behavior

After an ideal capacitor has finished charging from a steady DC source, no continuous DC current flows through its dielectric. A changing voltage, however, produces current. This is why capacitors can pass changing signals while blocking a steady DC level.

Capacitive reactance
XC = 1 / (2 π f C)

As frequency rises, capacitive reactance falls. A capacitor therefore presents a lower impedance to faster changes—until real-world parasitic inductance and losses become important.

For 1 µF at 1 kHz:
XC ≈ 159 Ω
Energy storage
E = 1/2 C V2

Stored energy increases directly with capacitance and with the square of voltage. Doubling voltage stores four times as much energy in the same capacitance.

Common circuit jobs
Decoupling

A capacitor near an integrated circuit supplies short bursts of local current and provides a low-impedance path for high-frequency noise. Small ceramic capacitors are commonly used close to device power pins, often with larger bulk capacitors elsewhere on the rail.

Coupling

A series capacitor can transfer an AC signal between amplifier stages while blocking a difference in DC bias voltage.

Filtering

Capacitors and resistors can form low-pass and high-pass networks. Power supplies use capacitors to reduce ripple, while signal circuits use them to shape frequency response.

Timing

The predictable charge and discharge of an RC network is used in delays, oscillators, pulse shaping, debouncing, and many simple timing circuits.

Before measuring capacitance or resistance in equipment, remove power and make sure stored charge has been safely discharged. A meter's capacitance range is not a discharge tool for a high-energy capacitor.