To find the current through the capacitor, we'll use the capacitor's voltage-current relationship, which states that the current is proportional to the rate of change of the voltage.
- Capacitor Voltage-Current Relationship: The current through a capacitor is given by \( i(t) = C \frac{dV(t)}{dt} \), where \( C \) is the capacitance and \( V(t) \) is the voltage.
- Capacitance (C): The property of a capacitor to store electrical energy, measured in Farads (F).
- Voltage (V(t)): The potential difference across the capacitor as a function of time.
- Current (i(t)): The flow of charge onto the capacitor plates as a function of time.
\( C = 0.5 \text{ F} \)
\( V(t)=\begin{cases} 0, & t<0 \\ 2t, & 02s \end{cases} \)
For \( t > 2s \), \( V(t) = 4e^{-(t-2)} \). Therefore, we need to find the derivative of \( V(t) \) with respect to \( t \):
\( \frac{dV(t)}{dt} = \frac{d}{dt} (4e^{-(t-2)}) = 4 \cdot \frac{d}{dt} (e^{-(t-2)}) = 4 \cdot (-1) e^{-(t-2)} = -4e^{-(t-2)} \)
Now, we can find \( i(t) \) using \( i(t) = C \frac{dV(t)}{dt} \):
\( i(t) = 0.5 \cdot (-4e^{-(t-2)}) = -2e^{-(t-2)} \)
The current \( i(t) \) for \( t > 2s \) is \( -2e^{-(t-2)} \).
Two batteries of emf's \(3V \& 6V\) and internal resistances 0.2 Ω \(\&\) 0.4 Ω are connected in parallel. This combination is connected to a 4 Ω resistor. Find:
(i) the equivalent emf of the combination
(ii) the equivalent internal resistance of the combination
(iii) the current drawn from the combination