Capacitor
In October 1745, Ewald Georg von Kleist of Pomerania, Germany, found that charge could be stored by connecting a high-voltage electrostatic generator by a wire to a volume of water in a hand-held glass jar
Pic-Glass jar
A capacitor essentially consists of two conducting surfaces separated by a layer of an insulating medium called a dielectric. The conducting surfaces may be in the form of either circular (or rectangular) plates or be of spherical or cylindrical shape. The purpose of a capacitor is to store electrical energy by electrostatic stress in the dielectric (the word ‘condenser is a misnomer since a capacitor does not ‘condense’ electricity as such, it merely stores it).
Capacitance
The property of a capacitor to ‘store electricity’ may be called
its capacitance.
similarly, the
capacitance of a capacitor is defined as “the amount of charge
required to create a unit potential difference between its plates.”
Suppose we give Q coulomb of charge to one of the two plates
of the capacitor and if a potential difference. of V volts is established between the two,
then its capacitance is
C =Q/V = Charge/Potential difference
Hence, capacitance is the charge required per unit potential difference.
By definition, the unit of capacitance is coulomb/volt which is also called farad (in honour of
Michael Faraday)
∴ 1 farad = 1 coulomb/volt
One farad is defined as the capacitance of a capacitor which requires a charge of one coulomb
to establish a p.d. of one volt between its plates.
One farad is actually too large for practical purposes. Hence, much smaller units like microfarad
(μF), nano-farad (nF), and micro-microfarad (μμF) or picofarad (pF) are generally employed.
Incidentally, capacitance is that property of a capacitor which delays and change of voltage
across it.
Different types of capacitors
- Fixed Capacitors
- Variable Capacitors
These two contain different types of capacitors including
- Non-polarized
- Polarized
Fixed capacitors of different types:
- Ceramic capacitors
- Electrolytic capacitors
- Film and paper capacitors
- Supercapacitors
- Glass, air-gap, vacuum, silicon, silver mica capacitors
Capacitors in Series
With reference to the Fig Series circuit,
let
C1, C2, C3 = Capacitances of three capacitors
V1, V2, V3 = p.ds. across three capacitors.
V = applied voltage across the combination
C = combined or equivalent or joining capacitance.
In series combination, the charge on all capacitors is the same but the potential difference across each is different.
∴ V = V1 + V2 + V3
or Q/C = Q/C1+Q/C2+Q/C3
or 1/C = 1/C1+1/C2+1/C3
For a changing applied voltage,
dV/dt = dV1/dt/dV2/dt dV3/dt
We can also find values of V1, V2, and V3 in terms of V.
Now, Q = C1V1 = C2V2 = C3V3 = CV
where C =(C1C2C3)/(C1C2+C2C3+C3C1) = (C1C2C3)/ (ΣC1C2)
∴ C1V1 = C V
or V1 = V(C1/C ) =V(C2C3)/ (ΣC1C2)
Similarly, V2 = =V(C1C3)/ (ΣC1C2)
V3 = =V(C1C2)/ (ΣC1C2)
Capacitors in Parallel
In this case, the potential difference across each is the same but the charge on each is different (Fig.Parallel Circuit).
∴ Q = Q1+Q2+Q3
or CV = C1V = C2V = C3V
or C = C1 + C2 + C3
For such a combination, dV/dt is the same for all capacitors.
Post a Comment