Capacitors
are passive devices used in electronic circuits to store energy in the form of an electric field. They are the compliment
of inductors, which store energy in the form of a magnetic field. An
ideal capacitor is the equivalent of an open circuit (infinite ohms) for direct currents (DC), and presents an impedance
(reactance) to alternating currents (AC) that depends on the frequency of the current (or voltage). The reactance
(opposition to current flow) of a capacitor is inversely proportional to the frequency of the of the signal acting
on it. Capacitors were originally referred to as "condensers" for a reason that goes back to the days of the Leyden
Jar where electric charges were thought to accumulate on plates through a condensation process.
The property of capacitance that opposes a change in voltage is exploited for the purpose of conducting signals
with a higher frequency component while preventing signals of lower frequency components from passing. A common
application of a capacitor in an RF (radio frequency) circuit is where there is a DC bias voltage that needs to
be blocked from being present in a circuit while allowing the RF signal to pass. DC power supplies use large capacitance
values in parallel with the output terminals to smooth out low frequency ripples due to rectification and/or switching
waveforms.
When used in series (left drawing) or
parallel (right drawing) with its circuit compliment, an inductor,
the inductorcapacitor combination forms a circuit that resonates at a particular frequency that depends on the
values of each component. In the series circuit, the impedance to current flow at the resonant frequency is zero
with ideal components. In the parallel circuit (right), impedance to current flow is infinite with ideal components.
Realworld capacitors made of physical components exhibit more than just a pure capacitance when
present
in an AC circuit. A common circuit simulator model is shown to the left. It includes the actual ideal capacitor
with a parallel resistive component ('Leakage') that responds to alternating current.
The equivalent DC resistive component ('ESR') is in series with the ideal capacitor
and an equivalent series inductive component ('ESL') is present due to metal leads
(if present) and characteristics of the plate surfaces. This inductance, in combination with the capacitance, creates
a resonant frequency at which point the capacitor looks like a pure resistance.
As the operational frequency is increased past resonance (aka selfresonant frequency,
or SRF), the circuit behaves as an inductance rather than a capacitance. Hence, careful consideration of
the SRF is required when selecting capacitors. SPICEtype simulators use this or an even more sophisticated model
to facilitate more accurate calculations over a wide range of frequencies.
Related Pages on RF Cafe  Capacitors &
Capacitance Calculations 
Capacitor
Color Codes  Capacitance Conversions 
Capacitor Dielectrics 
Standard Capacitor Values 
Capacitor Vendors 
The Noble Art of DeCoupling
Equations
for combining capacitors in series and parallel are given below. Additional equations are given for capacitors of
various configurations. As these figures and formulas indicate, capacitance is a measure of the ability of two surfaces
to store an electric charge. Separated and isolated by a dielectric (insulator), a net positive charge is accumulated
on one surface and a net negative charge is stored on the other surface. In an ideal capacitor, charge would be
stored indefinitely; however, real world capacitors gradually lose their charge due to leakage currents through
the nonideal dielectric.
Total capacitance of seriesconnected capacitors is equal to the reciprocal of the sum of the reciprocals
of the individual capacitances. Keep units constant.

Capacitance (C, in Farads) of two equalarea parallel plates is the product of the area (A, in meters)
of one plate, the distance (d, in meters) separating the plates, and the dielectric constant (ε,
in Farads per meter) of the space separating the plates. ε, the total dielectric constant, is the
product of the dielectric constant of free space, ε_{0}, and the relative dielectric constant
of the material, ε_{r}. Note that units of length and area can be metric or English so long
as they are consistent.




Dissipation
Factor (DF), aka Loss Tangent (tan δ) is interchangeably defined as the reciprocal of the charge (Q)
or the ratio of the equivalent series resistance (ESR) and the capacitive reactance (X_{C}). It
is a measure of the loss rate of stored charge. DF is typically used in low frequency applications while
tan δ is more often used in high frequency applications.


Total capacitance of parallelconnected capacitors is equal to the sum of the individual capacitances. Keep
units constant.

The following physical constants and mechanical dimensional variables apply to equations on this page.
Units for equations are shown inside brackets at the end of equations; e.g.,
means lengths are in inches and inductance is in Henries. If no units are indicated, then any may be used
so long as they are consistent across all entities; i.e., all meters, all µF, etc.
C = Capacitance L = Inductance W = Energy ε_{r} = Relative permittivity
(dimensionless) ε_{0} = 8.85 x 10^{12} F/m (permittivity
of free space) µ_{r} = Relative permeability (dimensionless) µ_{0}
= 4π x 10^{7}
H/m (permeability of free space)
1 meter = 3.2808 feet <—> 1 foot = 0.3048 meters 1 mm = 0.03937 inches <—>
1 inch = 25.4 mm
Also, dots (not to be confused with decimal points) are used to indicate
multiplication in order to avoid ambiguity.

Capacitive reactance (X_{C}, in Ω) is inversely proportional to the frequency (ω, in
radians/sec, or f, in Hz) and capacitance (C, in Farads). Pure capacitance has a phase angle of 90°
(voltage lags current with a phase angle of 90°).

Charge (Q, in coulombs) on a capacitor's plates is the product of the capacitance (C, in Farads) and the
voltage (V, in volts) across the device.

Energy (W, in Joules) stored in a capacitor is half the product of the capacitance (C, in Farads) and the
voltage (V, in volts) across the device.

Current does actually flow 'through' an ideal capacitor. Rather, charge stored on its plates is given up
to the connected circuit, thereby facilitating current flow. Conversely, a net voltage applied to its plates
causes a current to flow in the connected circuit as charge accumulates on the plates.

Quality factor is the dimensionless ratio of reactance to resistance in a capacitor.


