Solveeit Logo

Question

Question: A combination of parallel plate capacitors is maintained at a certain potential difference. When a \...

A combination of parallel plate capacitors is maintained at a certain potential difference. When a 3mm3mm thick slab is introduced between all the plates, in order to maintain the same potential difference, the distance between the plates is increased by 2.4mm2.4mm. Find the dielectric constant of the slab.

A. 44
B. 55
C. 33
D. 66

Explanation

Solution

Hint Find the equivalent capacitance both with and without the slab between the plates and equate them. Use suitable formula to establish the expression for capacitance.
Formulas used:
C=ε0AdC = \dfrac{{{\varepsilon _0}A}}{d} where dd is the distance between the capacitance plates, AA is the area of the plates and ε0{\varepsilon _0} is the permittivity of free space.
C=ε0Adt(11K)C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}} where KK is the relative permittivity of the material of the slab and dd'is the distance between the capacitor plates, tt is the thickness of the slab introduced.

Complete step by step answer
A capacitor is a system of conductors and dielectric that can store electric charge. It consists of two conductors containing equal and opposite charges and has a potential difference VV between them.
The potential difference between the conductors is proportional to the charge on the capacitor and is given by the relation Q=CVQ = CVwhere QQ is the charge on the positive conductor and CC is called the capacitance.
Now, we know that the potential difference between the two plates is given by, V=E×dV = E \times d where dd is the distance between the two plates.
Thus, substituting the value of VV in the equationQ=CVQ = CV, we get,
Q=CEdQ = CEd
Putting E=σε0E = \dfrac{\sigma }{{{\varepsilon _0}}} and σ=QA\sigma = \dfrac{Q}{A} where AA is the area of the capacitor plate, we get
Q=C×QAε0×dQ = C \times \dfrac{Q}{{A{\varepsilon _0}}} \times d
C=Aε0d\Rightarrow C = \dfrac{{A{\varepsilon _0}}}{d} where CC be the equivalent capacitance between terminals A and B.
Now, introducing a slab of thickness tt, the resultant capacitance CC' becomes
C=ε0Adt(11K)C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}} where KK is the relative permittivity of the material of the slab and dd'is the new distance between the capacitor plates.
Now, since the potential difference remains same, the capacitance must also not vary
So, C=CC = C'
Aε0d=Aε0dt(11K)\Rightarrow \dfrac{{A{\varepsilon _0}}}{d} = \dfrac{{A{\varepsilon _0}}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}
d=dt(11K) d=d+2.43(11K) 2.43+3K=0 3K=0.6 K=5  \Rightarrow d = d' - t\left( {1 - \dfrac{1}{K}} \right) \\\ \Rightarrow d = d + 2.4 - 3\left( {1 - \dfrac{1}{K}} \right) \\\ \Rightarrow 2.4 - 3 + \dfrac{3}{K} = 0 \\\ \Rightarrow \dfrac{3}{K} = 0.6 \\\ \Rightarrow K = 5 \\\

Therefore, the correct option is B.

Note: To establish the capacitance of an isolated single conductor, we assume the conductor to be a part of a capacitor whose other conductor is at infinity.