Step 1: Understanding the Concept:
A parallel plate capacitor consists of two large, flat, parallel conducting plates, each with an area A, separated by a small distance d. Capacitance (C) is a measure of its ability to store electric charge, defined as the ratio of the charge (Q) on one plate to the potential difference (V) between the plates.
Step 2: Derivation of the Expression:
Let the two plates of the capacitor have a surface charge density of \(+\sigma\) and \(-\sigma\). The charge on each plate is \(Q = \sigma A\).
Assuming the distance d is small compared to the dimensions of the plates, the electric field (\(E\)) between them is uniform and is given by:
\[ E = \frac{\sigma}{\epsilon_0} = \frac{Q}{A\epsilon_0} \]
where \(\epsilon_0\) is the permittivity of free space.
The potential difference (\(V\)) between the plates is the work done in moving a unit charge from one plate to another, which is \(V = E \times d\).
\[ V = \left(\frac{Q}{A\epsilon_0}\right)d = \frac{Qd}{A\epsilon_0} \]
The capacitance C is defined as \(C = \frac{Q}{V}\). Substituting the expression for V:
\[ C = \frac{Q}{\frac{Qd}{A\epsilon_0}} = \frac{A\epsilon_0}{d} \]
This is the expression for the capacitance of a parallel plate capacitor with a vacuum (or air) between the plates.
If a dielectric material with a dielectric constant K is inserted between the plates, the capacitance becomes:
\[ C = \frac{KA\epsilon_0}{d} \]
Step 3: How to Increase the Capacity:
Based on the formula \(C = \frac{KA\epsilon_0}{d}\), the capacitance can be increased in the following ways:
\begin{enumerate}
\item By increasing the area of the plates (A): Capacitance is directly proportional to the area of the plates.
\item By decreasing the distance between the plates (d): Capacitance is inversely proportional to the separation between the plates.
\item By introducing a dielectric medium: Inserting a dielectric material with a high dielectric constant (K > 1) between the plates increases the capacitance by a factor of K.
\end{enumerate}
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