A capacitor of capacitance 100 μF is charged to a potential of 12 V and connected to a 6.4 mH inductor to produce oscillations. The maximum current in the circuit would be:
The maximum current in the LC circuit can be determined using energy conservation. Initially, the capacitor stores energy, calculated as \(E_{\text{cap}} = \frac{1}{2} C V^2\). With \(C = 100 \, \mu \text{F} = 100 \times 10^{-6} \, \text{F}\) and \(V = 12 \, \text{V}\), the initial capacitor energy is:
\(E_{\text{cap}} = \frac{1}{2} \times 100 \times 10^{-6} \times (12)^2 = 0.0072 \, \text{J}\)
In an LC circuit, this maximum capacitor energy equals the maximum inductor energy when the capacitor is discharged. The inductor energy is given by \(E_{\text{ind}} = \frac{1}{2} L I_{\text{max}}^2\). Equating these energies:
\(\frac{1}{2} L I_{\text{max}}^2 = 0.0072\)
Given \(L = 6.4 \, \text{mH} = 6.4 \times 10^{-3} \, \text{H}\), we solve for \(I_{\text{max}}\):
\(\frac{1}{2} \times 6.4 \times 10^{-3} \times I_{\text{max}}^2 = 0.0072\)
\(I_{\text{max}}^2 = \frac{0.0072 \times 2}{6.4 \times 10^{-3}} = 2.25\)
\(I_{\text{max}} = \sqrt{2.25} = 1.5 \, \text{A}\)
Therefore, the maximum current in the circuit is 1.5 A.
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.