A parallel plate capacitor consists of a plate connected to a positive end of a cell and another plate connected to the negative end or earthed. But let us first understand what is meant by a capacitor. A capacitor consists of 2 conducting surfaces that are separated by a layer of an insulating medium also called a dielectric. This dielectric can be any insulating medium, the most common being parallel plate capacitors with air between the plates. The capacity of a conductor can be defined as the ratio between the charge on the conductor to its potential.
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C=Q/V, where C is the capacitance of the parallel plate capacitor, ( equation-1)
Q is the charge on the plates and V is the potential between the plates.
However, the capacitance of a parallel plate capacitor depends on its geometrical shape. We will discuss this later in this article regarding how a parallel plate capacitor of capacitance c depends on the distance between plates and the area of the plates.
Also, check-
See the figure of a parallel plate capacitor with air in between the plates-
(Fig-1)
It is experimentally found that in presence of an earthed plate (see fig-2), the other plate is capable of withdrawing more charge than when it is not. When a parallel plate capacitor is charged by a battery, there is a momentary flow of electrons from one plate to another. As electrons (negative charges) are withdrawn from the first plate, it becomes positively charged and the electrons get collected on the second plate which becomes negatively charged forming a potential difference between the two plates.
Thus, there is a transient flow of electrons giving rise to a charging current and this charging current is maximum when the 2 plates are uncharged. This charging current keeps decreasing and finally becomes 0 when the potential difference between plates becomes equal and opposite to the applied battery emf.
The principle of the parallel plate capacitor is based on the fact that when an earthed conductor is placed in the neighbourhood of a charged conductor, the capacity of the parallel plate capacitor system increases considerably. Let a plate is connected to cell. After V of cell and plate becomes equal, no more charge can be put into the plate. However, if we put another plate of opposite charge parallel to it, V decreases ( since V is added algebraically, therefore V decreases in the first plate). That’s why more charges start flowing and we say that capacity of the plate increases. Thus the property of a capacitor is to store charges and this property is called capacitance.
NCERT Physics Notes:
In S.I. unit, capacitance is measured in Farad (F).
1F=1Coulomb of charge/1 volt of potential
(By equation 1) we can define 1 Farad as - the capacity of a conductor is 1F, if a charge of 1 Coulomb is required to establish a p.d. of 1 Volt between the plates.
In C.G.S. unit, capacitance is measured in stat farad.
Dimensional formula of capacitance is [M-1L-2T4A2].
(Fig-3)
Q=σA and E=σ/ϵ0 (for sheets of charges)
E=Q/(Aϵ0)
Since, E=V/d (magnitudically) => V/d=Q/(Aϵ0)
Q/V=Aϵ0/d
C=Aϵ0/d - (equation 2)
So, here parallel plate capacitance C depends on geometrical shape i.e. the distance between the 2 plates or the plate separation d, parallel plate capacitor of area A and ϵ0.
Generally, we need 2 identical parallel plate capacitors i.e. the area A of plates should be taken equal because if one is smaller and the other is bigger, only the smaller part of the plate is useful, the extra part becomes useless.
The capacitance of parallel plate capacitor with the dielectric slab in between with dielectric constant K is-
C=Aϵ0K/d - (equation 3)
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Series Combination- In a series combination, each capacitor is charged with the same charge while they will be raised through different potentials in accordance with their capacities.
Let V1=potential across C1
V2= potential across C2 and so on.
Q=charge given to each capacitor
Since Q=CV
Therefore Q=C1V1, Q=C2V2, ….. and so on.
Total potential = V=V1+V2+….. = Q/C1+Q/C2+……
Q/C=Q/C1+Q/C2+……
1/Ceff=1/C1+1/C2+….. This is the formula for total capacitance in a series combination. (equation 5)
Also read :
Parallel Combination - The capacitors are said to be connected in parallel combination between any 2 points if we can proceed from 1 point to another along different paths. Since the capacitances are joined through 2 common points, V is constant in all of them.
Q1=C1V, Q2=C2V,……
Since charges can be added algebraically, we get-
Qtot=Q1+Q2+…
Ceff=C1V+C2V+…
Ceff = C1+C2+… (equation 6)
Let capacitance of the capacitor be C charged by a cell of potential difference V. Let v be the potential between plates of the capacitor at any instant of time.
U=CV2/2 (equation 7)
The above equation represents the force between the plates of a parallel plate capacitor charged to a potential difference of V. The negative sign implies the force is an attractive force.
Also read -
C=C1C2/(C1+C2) = 10×20/(10+20)=6.6 μF
Energy stored in the capacitor=area under given plot=(1/2)QV
It is the ratio of capacitance Cd of the capacitor with the dielectric as the medium to its capacitance Cv i.e. when capacitors are in vacuum.
K=Cd/Cv
Parallel plate circuits block DC current when placed in circuits.
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