\(\frac{1}{2}\)
\(\frac{1}{3}\)
\(\frac{1}{4}\)
\(\frac{1}{6}\)
To solve this problem, we need to consider the discharge behavior of a capacitor through a resistor. The energy stored in a capacitor and the charge stored decay exponentially over time when the capacitor discharges through a resistor.
The energy stored in a capacitor is given by:
E = \frac{1}{2}C V^2
where \( C \) is the capacitance and \( V \) is the voltage across the capacitor.
When a capacitor discharges, the energy decreases as:
E(t) = E_0 e^{-2t/RC}
E_0 is the initial energy.
The charge on the capacitor at any time is given by:
Q(t) = Q_0 e^{-t/RC}
Q_0 is the initial charge.
Let's consider:
Using the energy decay equation:
\frac{1}{2}E_0 = E_0 e^{-2t_1/RC}
\Rightarrow e^{-2t_1/RC} = \frac{1}{2}
Taking logarithm on both sides:
-\frac{2t_1}{RC} = \ln \left(\frac{1}{2}\right)
t_1 = \frac{RC}{2} \ln(2)
Using the charge decay equation:
\frac{1}{8}Q_0 = Q_0 e^{-t_2/RC}
\Rightarrow e^{-t_2/RC} = \frac{1}{8}
Taking logarithm on both sides:
-\frac{t_2}{RC} = \ln \left(\frac{1}{8}\right)
t_2 = RC \ln(8)
Now, we find the ratio \frac{t_1}{t_2}:
\frac{t_1}{t_2} = \frac{\frac{RC}{2}\ln(2)}{RC\ln(8)}
\Rightarrow \frac{t_1}{t_2} = \frac{1}{2} \times \frac{\ln(2)}{\ln(8)}
Since \ln(8) = \ln(2^3) = 3\ln(2), we substitute:
\frac{t_1}{t_2} = \frac{1}{2} \times \frac{\ln(2)}{3\ln(2)}
\Rightarrow \frac{t_1}{t_2} = \frac{1}{6}
Thus, the ratio \frac{t_1}{t_2} is \frac{1}{6}, which corresponds to 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.