Answer
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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:
$C = \dfrac{{{\varepsilon _0}A}}{d}$ where $d$ is the distance between the capacitance plates, $A$ is the area of the plates and ${\varepsilon _0}$ is the permittivity of free space.
$C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$ where $K$ is the relative permittivity of the material of the slab and $d'$is the distance between the capacitor plates, $t$ 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 $V$ between them.
The potential difference between the conductors is proportional to the charge on the capacitor and is given by the relation $Q = CV$where $Q$ is the charge on the positive conductor and $C$ is called the capacitance.
Now, we know that the potential difference between the two plates is given by, $V = E \times d$ where $d$ is the distance between the two plates.
Thus, substituting the value of $V$ in the equation$Q = CV$, we get,
$Q = CEd$
Putting $E = \dfrac{\sigma }{{{\varepsilon _0}}}$ and $\sigma = \dfrac{Q}{A}$ where $A$ is the area of the capacitor plate, we get
$Q = C \times \dfrac{Q}{{A{\varepsilon _0}}} \times d$
$ \Rightarrow C = \dfrac{{A{\varepsilon _0}}}{d}$ where $C$ be the equivalent capacitance between terminals A and B.
Now, introducing a slab of thickness $t$, the resultant capacitance $C'$ becomes
$C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$ where $K$ is the relative permittivity of the material of the slab and $d'$is the new distance between the capacitor plates.
Now, since the potential difference remains same, the capacitance must also not vary
So, $C = C'$
$ \Rightarrow \dfrac{{A{\varepsilon _0}}}{d} = \dfrac{{A{\varepsilon _0}}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$
$
\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.
Formulas used:
$C = \dfrac{{{\varepsilon _0}A}}{d}$ where $d$ is the distance between the capacitance plates, $A$ is the area of the plates and ${\varepsilon _0}$ is the permittivity of free space.
$C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$ where $K$ is the relative permittivity of the material of the slab and $d'$is the distance between the capacitor plates, $t$ 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 $V$ between them.
The potential difference between the conductors is proportional to the charge on the capacitor and is given by the relation $Q = CV$where $Q$ is the charge on the positive conductor and $C$ is called the capacitance.
Now, we know that the potential difference between the two plates is given by, $V = E \times d$ where $d$ is the distance between the two plates.
Thus, substituting the value of $V$ in the equation$Q = CV$, we get,
$Q = CEd$
Putting $E = \dfrac{\sigma }{{{\varepsilon _0}}}$ and $\sigma = \dfrac{Q}{A}$ where $A$ is the area of the capacitor plate, we get
$Q = C \times \dfrac{Q}{{A{\varepsilon _0}}} \times d$
$ \Rightarrow C = \dfrac{{A{\varepsilon _0}}}{d}$ where $C$ be the equivalent capacitance between terminals A and B.
Now, introducing a slab of thickness $t$, the resultant capacitance $C'$ becomes
$C' = \dfrac{{{\varepsilon _0}A}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$ where $K$ is the relative permittivity of the material of the slab and $d'$is the new distance between the capacitor plates.
Now, since the potential difference remains same, the capacitance must also not vary
So, $C = C'$
$ \Rightarrow \dfrac{{A{\varepsilon _0}}}{d} = \dfrac{{A{\varepsilon _0}}}{{d' - t\left( {1 - \dfrac{1}{K}} \right)}}$
$
\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.
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