To find the electrostatic energy of the system, we need to consider both the capacitor with and without the dielectric. First, calculate the capacitance without the dielectric. The formula for the capacitance C of a parallel plate capacitor is:
C = (ε0 * A) / d
where A is the area of the plate and d is the separation between the plates.
The area A of the capacitor is:
A = width * length = 0.04 m * 0.08 m = 0.0032 m²
The separation d is 4 mm = 0.004 m.
Thus, the capacitance C is:
C = (ε0 * 0.0032) / 0.004 = 0.8 ε0
Next, consider the dielectric slab. It covers an area Ad (area with the dielectric) and has a thickness equal to the separation.
The area Ad is:
Ad = width * length of dielectric = 0.04 m * 0.01 m = 0.0004 m²
The remaining area without dielectric is:
Ar = total area - Ad = 0.0032 m² - 0.0004 m² = 0.0028 m²
The capacitance with the dielectric C1 is:
C1 = (5ε0 * Ad) / d = (5ε0 * 0.0004) / 0.004 = 0.5 ε0
The capacitance without the dielectric C2 is:
C2 = (ε0 * Ar) / d = (ε0 * 0.0028) / 0.004 = 0.7 ε0
The total capacitance Ctotal is the sum:
Ctotal = C1 + C2 = 0.5 ε0 + 0.7 ε0 = 1.2 ε0
The energy U stored in the capacitor is given by:
U = 0.5 * Ctotal * V²
where V = 20 V. Thus,
U = 0.5 * 1.2 ε0 * 20² = 240 ε0
The electrostatic energy of the system is 240 ε0 J, which is within the given range of 240,240.
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.