To solve this problem, we need to find the dielectric constant of the material between the plates of the capacitor. Let's go through the problem step-by-step:
Calculating the values: \varepsilon_r = \frac{Q \cdot 4\pi \cdot 9 \times 10^9}{30\pi \times 10^{-4} \times 3.6 \times 10^7}
This simplifies to: \varepsilon_r = 2.33
Therefore, the dielectric constant of the material is 2.33, which matches the correct answer.
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.