The system's capacitance \( C \) is determined by the formula \( C = \frac{Q}{V} \), with \( Q = 80 \, \mu C = 80 \times 10^{-6} \, C \) and \( V = 16 \, \text{V} \). This yields a capacitance of \( C = \frac{80 \times 10^{-6}}{16} = 5 \, \mu F \).
(ii) Introducing a dielectric with constant \( k = 3 \) increases the capacitance by a factor of \( k \), resulting in a new capacitance \( C' = kC = 3 \times 5 \, \mu F = 15 \, \mu F \). Since \( Q = C'V' \) and \( Q \) is constant, the new potential difference is \( V' = \frac{Q}{C'} = \frac{80 \times 10^{-6}}{15 \times 10^{-6}} = 5.33 \, \text{V} \).
(iii) The capacitance of the system is solely dependent on the conductor geometry and the dielectric constant of the intervening medium, not the charges. Therefore, doubling the charges does not alter the capacitance, which remains \( 5 \, \mu F \) as capacitance is independent of charge.
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.