To find the permittivity of the dielectric medium used in the parallel plate capacitor, we need to understand the relationship between the initial and final capacitance, and the properties of the dielectric material introduced.
The capacitance of a parallel plate capacitor with air (or vacuum) as the dielectric medium is given by:
\(C_0 = \frac{\epsilon_0 \cdot A}{d}\)
where \(\epsilon_0 = 8.85 \times 10^{-12} \, C^2 N^{-1}m^{-2}\) is the permittivity of free space, \(A\) is the plate area, and \(d\) is the separation between the plates.
When a dielectric medium is introduced, the capacitance increases by a factor known as the dielectric constant (or relative permittivity \(\kappa\) of the medium:
\(C = \kappa \cdot C_0\)
We are given:
Thus, the dielectric constant \(\kappa\) can be calculated as:
\(\kappa = \frac{C}{C_0} = \frac{30 \times 10^{-6}}{6 \times 10^{-6}} = 5\)
The permittivity of the dielectric medium, \(\epsilon\), is given by:
\(\epsilon = \kappa \cdot \epsilon_0\)
Substituting the known values:
\(\epsilon = 5 \cdot 8.85 \times 10^{-12} \, C^2 N^{-1}m^{-2} = 44.25 \times 10^{-12} \, C^2 N^{-1}m^{-2}\)
Converting this into the required form:
\(\epsilon = 4.425 \times 10^{-11} \, C^2 N^{-1}m^{-2} = 0.4425 \times 10^{-10} \, C^2 N^{-1}m^{-2}\)
Upon converting this to the closest given option:
Thus, the permittivity of the medium is 0.44 × 10-10 C2 N-1m-2, which matches with \(0.44 \times 10^{-10} \, C^2 N^{-1}m^{-2}\) from the given options.
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.