Rankers Physics

Capacitor With Dielectrics: Practice Problem & Solution

An isolated parallel-plate capacitor consists of two metal plates of area A and separation d. A slab of thickness t and dielectric constant K = 2 is inserted between the plates with its faces parallel to the plates and having the same surface area as that of the plates as shown Capacitor With Dielectrics diagram: An isolated parallel-plate capacitor consists of two metal The capacitance of the system is :  
\[\frac{\varepsilon_{0}A}{\left( d-\frac{t}{2} \right)}\]
\[\frac{\varepsilon_{0}A}{\left( d+\frac{t}{2} \right)}\]
\[\frac{\varepsilon_{0}A}{d-t}\]
\[\frac{\varepsilon_{0}A}{d+t}\]

Short Solution (Best for NEET):

To solve this problem, we apply the core principles of Capacitor With Dielectrics. Understanding the underlying formula is key to arriving at the correct answer below:

The question involves calculating the capacitance of a parallel-plate capacitor when a dielectric slab of thickness

tt

and dielectric constant

K=2K = 2

is partially inserted between the plates.

The short solution is based on treating the system as a combination of two capacitors in series:

  1. Capacitor 1 (region with dielectric): The thickness of this region is
    tt
     

    , and the capacitance is given by: 

    C1=ε0AKt=2ε0AtC_1 = \frac{\varepsilon_0 A K}{t} = \frac{2\varepsilon_0 A}{t} 

  2. Capacitor 2 (region without dielectric): The thickness of this region is
    d−td - t
     

    , and the capacitance is: 

    C2=ε0Ad−tC_2 = \frac{\varepsilon_0 A}{d - t} 

Since the two regions are in series, the equivalent capacitance is given by:

 

1C=1C1+1C2\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2}

 

Substituting

C1C_1

and

C2C_2

:

 

1C=t2ε0A+d−tε0A\frac{1}{C} = \frac{t}{2\varepsilon_0 A} + \frac{d - t}{\varepsilon_0 A}

 

Simplifying:

 

1C=t+2(d−t)2ε0A=2d−t2ε0A\frac{1}{C} = \frac{t + 2(d - t)}{2\varepsilon_0 A} = \frac{2d - t}{2\varepsilon_0 A}

 

Therefore:

 

C=2ε0A2d−tC = \frac{2\varepsilon_0 A}{2d - t}

 

When the dielectric slab thickness is

t=d2t = \frac{d}{2}

, the capacitance simplifies to:

 

C=ε0Ad−t2C = \frac{\varepsilon_0 A}{d - \frac{t}{2}}

 

This matches the given answer. Let me know if further clarification is needed!

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