To understand the effect of introducing a dielectric slab between the plates of a capacitor while it is connected to a battery, we need to analyze the behavior of the capacitor's parameters such as charge, potential difference, energy, and capacitance.
Let's consider a parallel plate capacitor with capacitance \(C_0\) when the dielectric constant is 1 (i.e., in vacuum or air). The capacitance is given by:
\(C_0 = \frac{\varepsilon_0 A}{d}\)
where:
When a dielectric slab with dielectric constant \(\kappa\) is introduced between the plates, the capacitance becomes:
\(C = \kappa C_0 = \kappa \frac{\varepsilon_0 A}{d}\)
Since the capacitor is connected to a battery, the potential difference \(V\) across the capacitor remains constant. Consequently, according to the relation between charge \(Q\), capacitance \(C\), and potential difference \(V\):
\(Q = CV\)
When the capacitance increases from \(C_0\) to \(C\), and since \(V\) is constant, the charge on the capacitor also increases. Thus, the charge \(Q\) becomes:
\(Q' = \kappa C_0 V = \kappa Q\)
This implies the charge on the capacitor increases.
Let’s examine the given options:
Thus, the correct answer is charge on capacitor increases.
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.