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The Parallel Plate Capacitor

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Estimated time: 5 minutes
CBSE: Class 12

Definition: The Parallel Plate Capacitor

A capacitor that consists of two large, parallel, conducting plates separated by a small distance is called a parallel plate capacitor.

CBSE: Class 12

Formula: Capacitance of a Parallel Plate Capacitor

For two plates separated by distance d:

\[C=\frac{\varepsilon_0A}{d}\]

With a dielectric medium:

\[C=\frac{K\varepsilon_0A}{d}\]

CBSE: Class 12

Step-by-Step Derivation of Capacitance

Step 1: Surface Charge Density

σ = \[\frac {Q}{A}\]

Step 2: Electric Field Between the Plates

Using the result from Gauss's Law for a large sheet of charge, the electric field due to each plate is \[\frac {σ}{2ε_0}\]. For two plates with opposite charges, both contributions add between the plates:

E = \[\frac {σ}{ε_0}\] = \[\frac {Q}{ε_0A}\]

Outside the plates, the fields are equal and opposite → they cancel → E = 0 outside.

Step 3: Potential Difference Between the Plates

V = E ⋅ d = \[\frac {Q⋅d}{ε_0A}\]

Step 4: Capacitance

C = \[\frac {Q}{V}\] = \[\frac{Q}{\frac{Qd}{\varepsilon_0A}}\]
 
Result:
C = \[\frac {ε_0A}{d}\]

Capacitance depends only on geometry (A and d) and the medium — NOT on Q or V.

CBSE: Class 12

Factors Affecting Capacitance

Factor Effect on Capacitance (C) Reason
Increase plate area (A) Capacitance increases (C ∝ A) A larger plate area allows more charge to be stored for the same potential difference.
Increase plate separation (d) Capacitance decreases ((C ∝ 1/d)) Greater separation reduces the electric field interaction between the plates.
Insert a dielectric (K > 1) Capacitance increases (C = Kε0A/d) The dielectric reduces the effective electric field, enabling more charge storage.
Change charge (Q) or potential difference (V) No effect on capacitance Capacitance depends only on the geometry of the conductors and the dielectric medium.
CBSE: Class 12

Effect of Dielectric

When a dielectric slab of dielectric constant K is inserted between the plates:

Formula with Dielectric:

C = \[\frac {Kε_0A}{d}\]
  • The electric field is reduced to E′ = \[\frac {E}{K}\] due to polarisation of the dielectric
  • Since V′ = E′ ⋅ d decreases, and C = Q/V′, the capacitance increases by factor K

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