The objective is to determine the supply voltage applied to a parallel plate capacitor that has been modified with dielectric materials. The initial capacitance and dimensions, the dielectric constants of the new materials, and the resultant attractive force between the plates are provided.
The solution employs several fundamental concepts from electrostatics:
Step 1: Enumerate the given parameters and model the new capacitor configuration.
The modified capacitor can be analyzed as two capacitors connected in parallel. \(C_1\) represents the capacitor with dielectric \(K_1\) and area \(A/2\), and \(C_2\) represents the capacitor with \(K_2\) and area \(A/2\).
Step 2: Compute the new equivalent capacitance \(C_{\text{new}}\).
The capacitance of the original air-filled capacitor is \(C_{\text{air}} = \frac{\epsilon_0 A}{d}\).The capacitances of the two new segments are:
\[C_1 = \frac{K_1 \epsilon_0 (A/2)}{d} = \frac{K_1}{2} \left(\frac{\epsilon_0 A}{d}\right) = \frac{K_1}{2} C_{\text{air}}\]\[C_2 = \frac{K_2 \epsilon_0 (A/2)}{d} = \frac{K_2}{2} \left(\frac{\epsilon_0 A}{d}\right) = \frac{K_2}{2} C_{\text{air}}\]Since these two segments are in parallel, the new equivalent capacitance is their sum:
\[C_{\text{new}} = C_1 + C_2 = \frac{K_1}{2} C_{\text{air}} + \frac{K_2}{2} C_{\text{air}} = \frac{C_{\text{air}}}{2} (K_1 + K_2)\]Step 3: Substitute the given values to determine the numerical value of \(C_{\text{new}}\).
\[C_{\text{new}} = \frac{10 \times 10^{-6} \, \text{F}}{2} (2 + 3)\]\[C_{\text{new}} = (5 \times 10^{-6}) \times 5 = 25 \times 10^{-6} \, \text{F} = 25 \, \mu\text{F}\]Step 4: Employ the force formula to calculate the supply voltage \(V\).
The relationship between force, capacitance, voltage, and plate separation is given by:
\[F = \frac{1}{2d} C_{\text{new}} V^2\]Rearrange this equation to solve for voltage \(V\):
\[V^2 = \frac{2Fd}{C_{\text{new}}}\]\[V = \sqrt{\frac{2Fd}{C_{\text{new}}}}\]Step 5: Substitute the known values and compute the final voltage.
\[V = \sqrt{\frac{2 \times 8 \, \text{N} \times (10 \times 10^{-3} \, \text{m})}{25 \times 10^{-6} \, \text{F}}}\]\[V = \sqrt{\frac{160 \times 10^{-3}}{25 \times 10^{-6}}} = \sqrt{\frac{160}{25} \times 10^3}\]\[V = \sqrt{6.4 \times 1000} = \sqrt{6400}\]\[V = 80 \, \text{V}\]The required supply voltage is 80 V.
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.