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Capacitance of a Parallel-Plate Capacitor with Dielectric Slab between Plates

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Estimated time: 10 minutes
CISCE: Class 12

Introduction

Think of the dielectric as a "traffic buffer." When a slab is inserted between the plates, its molecules align and create an internal field that opposes part of the original field — like a crowd partially blocking wind flow through a corridor. This reduces the net electric field inside the slab region, which lowers the voltage needed for the same charge, and since C = q/V, a lower V for the same q means higher C.

CISCE: Class 12

Derivation

Setup: Parallel plates of area A, separated by distance d, carrying charge q. A dielectric slab of thickness t (where t < d) and dielectric constant K is placed between the plates.

Step 1 - Field without dielectric (in the air gap):

  • E0 = \[\frac {q}{ε_0A}\]

Step 2 - Field inside the dielectric (reduced by K):

  • E = \[\frac {q}{Kε_0A}\]

Step 3 - Total potential difference across the capacitor:

  • V = \[\frac {q}{ε_0A}\](d − t) + \[\frac {q}{Kε_0A}\]t

Step 4 - Capacitance from C = q/V:

  • C = \[\frac {ε_0A}{d−t+\frac {t}{K}}\]
CISCE: Class 12

Special Cases

Case Condition Resulting Formula Notes
No dielectric (air only) t = 0 C = \[\frac {ε_0A}{d}\] Standard air capacitor formula
Dielectric fills entire gap t = d C = \[\frac {Kε_0A}{d}\] Maximum enhancement by factor K
Metal slab inserted K → ∞ C = \[\frac {ε_0A}{d−t}\] Metal has zero internal field; conducting slab acts like reduced gap
Metal slab fills entire gap t = d, K → ∞ C → ∞ Idealised limit — not physically realisable
CISCE: Class 12

Multiple Dielectric Slabs

When several dielectric slabs of thicknesses t1, t2, t3,… and constants K1, K2, K3,… are stacked between the plates, each acts like a capacitor in series:

  • C = \[\frac{\varepsilon_0A}{(d-t_1-t_2-\cdots)+\frac{t_1}{K_1}+\frac{t_2}{K_2}+\cdots}\]
Slab Thickness Dielectric Constant Contribution to denominator
Slab 1 t1 K1 t1/K1
Slab 2 t2 K2 t2/K2
Remaining air gap d − ∑ti​ 1 (air) d − ∑ti
CISCE: Class 12

Example

Simple explanation: A 3.0 mm dielectric slab is inserted between capacitor plates, and the plate separation must increase by 2.4 mm to keep the voltage the same — this tells us the slab's dielectric constant is 5.

Why it happens: Inserting a dielectric slab reduces the field inside it, which lowers the voltage. To bring the voltage back to its original value, you must move the plates farther apart—this compensates for the slab's field-weakening effect.

Steps in the solution:

  • Originally, without any slab, the voltage is simply field × distance: V0 = E0d.

  • After inserting the slab (thickness t) and increasing the gap by d', the new voltage equation has two parts: the air gap contributes E0(d + d′ − t), and the slab region contributes E0t/K (weaker field inside dielectric).

  • Since both expressions equal the same V0​, they are set equal to each other and simplified.

  • This simplification directly gives K = \[\frac {t}{t−d′}\].

  • Plugging in the numbers: K = \[\frac {3.0}{3.0−2.4}\] = \[\frac {3.0}{0.6}\] = 5.

Answer: The dielectric constant of the slab is K = 5.

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