A capacitor
is a passive element designed to store energy in its electric field. It
generally consists of two conducting plates separated by an insulator (or
dielectric).
WHAT HAPPENS IN A CAPACITOR?
When a
voltage source ‘v’ is connected to a capacitor, the source deposits positive
charge q on one plate and a negative charge –q on the other plate. The
capacitor is said to store the electric charge. The amount of charge stored is
given by
\[q=Cv\]
Where, C – constant of proportionality
v – Voltage applied
The unit of capacitance is farad (F), in honor of English physicist Michael Faraday (1791-1867). For a parallel plate capacitor, capacitance is given by
\[C=\in
\frac{A}{d}\]
Where, A- surface area of the plates
d- Distance between the plates
$\in $- Permittivity of the
material
TYPES OF CAPACITORS –
Capacitors
are of two types based on their functioning:-
- Fixed
- Variable
The symbols
for fixed and variable type capacitors are shown in the figure below.
The figure below shows common types of fixed value capacitors. Polyester
capacitors are light in weight, stable and their change with temperature is
predictable. Other dielectrics such as mica or polystyrene may be used. Film
capacitors are rolled and housed in metal or plastic films. Electric capacitors
produce very high capacitances.
FIXED CAPACITORS:- (a) Polyester (b) Ceramic (c) Electrolytic |
VARIABLE CAPACITORS:- (a) Trimmer (b) Filmtrim |
USES OF CAPACITOR –
Besides resistors,
capacitors are the most common electrical components. They are used extensively
in electronics, communication, computers, and power systems. They are used in
tuning circuits and as dynamic memory elements in computer.
Capacitors
are also used to block dc, pass ac, shift phase, start motors and suppress
noise.
ENERGY STORED IN A CAPACITOR –
We know
that, $q=Cv$
Differentiating
this, we get $\frac{dq}{dt}=C\frac{dv}{dt}$
or $i=C\frac{dv}{dt}$ (Since, $i=\frac{dq}{dt}$ )
Integrating
this, $v=\frac{1}{C}\int\limits_{-\infty }^{t}{idt}$
Or
\[v=\frac{1}{C}\int\limits_{{{t}_{0}}}^{t}{idt+v({{t}_{0}})}\]
V(t0)
is the voltage across the capacitor at time t0. This shows that the
capacitor voltage depends on the past history of the capacitor current.
Instantaneous
power delivered to the capacitor is $p=vi=Cv\frac{dv}{dt}$
Therefore,
energy stored is
\[w=\int\limits_{-\infty
}^{t}{pdt}=C\int\limits_{-\infty }^{t}{v\frac{dv}{dt}dt}=C\int\limits_{-\infty
}^{t}{vdv}=\frac{1}{2}C{{v}^{2}}\]
V ($-\infty $) =0, because the capacitor was
not charged at t=$-\infty $
Thus,
\[w=\frac{1}{2}C{{v}^{2}}\text{
or }w=\frac{{{q}^{2}}}{2C}\]
PROPERTIES OF A CAPACITOR –
- When the voltage across a capacitor is not changing with time (i.e. dc voltage), the current through the capacitor is zero.A capacitor is an open circuit to dc. With dc voltage connected across a capacitor, it charges.
- The voltage on the capacitor must be
continuous. The voltage on the capacitor cannot change abruptly because an
abrupt change would mean an infinite current, which is physically impossible. Conversely, the current through a capacitor can change instantaneously.
VOLTAGE ACROSS A CAPACITOR (a) possible (b) not possible - An ideal capacitor does not dissipate energy.
- A real, non-ideal capacitor has a
parallel-model leakage resistance as shown in figure. The leakage resistance
may be as high as 100M$\Omega $ and can
be neglected for most practical applications.
CIRCUIT MODEL OF A NON-IDEAL CAPACITOR