1. Initial Conditions:
The initial capacitance is \( C_0 = 12.5 \, \text{pF} \), and the initial charge on the capacitor is \( Q = C_0V \).
2. Capacitance After Dielectric Insertion:
Upon inserting a dielectric with a dielectric constant of \( \epsilon_r = 6 \), the capacitance changes to:
\[ C_f = \epsilon_r C_0. \]
3. Change in Potential Energy:
The potential energy change is calculated as:
\[ \Delta U = U_i - U_f = \frac{Q^2}{2C_i} - \frac{Q^2}{2C_f}. \] Using \( Q = C_0V \) and simplifying:
\[ \Delta U = \frac{(C_0V)^2}{2C_0} \left[ 1 - \frac{1}{\epsilon_r} \right] = \frac{1}{2} C_0V^2 \left[ 1 - \frac{1}{6} \right]. \]
4. Calculation:
With \( C_0 = 12.5 \, \text{pF}, \, V = 12 \, \text{V}, \, \text{and} \, \epsilon_r = 6 \), the calculation is:
\[ \Delta U = \frac{1}{2} \times 12.5 \times 10^{-12} \times (12)^2 \times \frac{5}{6}. \] The simplified result is:
\[ \Delta U = 750 \, \text{pJ} = 750 \times 10^{-12} \, \text{J}. \]
Answer: \( 750 \times 10^{-12} \, \text{J} \)
A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit. 
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.