To solve for the current through an inductor given the voltage across it, we use the inductor's voltage-current relationship.
- Inductor Voltage-Current Relationship: The voltage across an inductor is given by \( V(t) = L \frac{di(t)}{dt} \), where \( L \) is the inductance and \( i(t) \) is the current.
- Inductance (L): The property of an inductor to oppose changes in current, measured in Henrys (H).
- Voltage (V(t)): The potential difference across the inductor as a function of time.
- Current (i(t)): The flow of charge through the inductor as a function of time.
\( V(t) = 15e^{-5t} \text{ V} \)
\( L = 212 \text{ mH} = 0.212 \text{ H} \)
We need to find \( i(t) \) given \( V(t) = L \frac{di(t)}{dt} \). Rearranging for \( di(t) \) gives us \( di(t) = \frac{V(t)}{L} dt \). Now, we integrate both sides with respect to time:
\( i(t) = \int \frac{V(t)}{L} dt = \int \frac{15e^{-5t}}{0.212} dt = \frac{15}{0.212} \int e^{-5t} dt \)
\( i(t) = \frac{15}{0.212} \cdot \frac{e^{-5t}}{-5} + C = -\frac{15}{0.212 \times 5} e^{-5t} + C = -\frac{3}{0.212} e^{-5t} + C \)
\( i(t) = -14.15 e^{-5t} + C \)
Assuming the initial current \( i(0) = 0 \), then \( 0 = -14.15 e^{0} + C \)
so \( C = 14.15 \). Therefore, \( i(t) = -14.15e^{-5t} + 14.15 = 14.15(1-e^{-5t}) \)
Based on the options, is: \( 14.15e^{-5t} \) . If the intial condition is i(0) = 0, then the final answer would be $14.15(1-e^{-5t})$.
In the given circuit the sliding contact is pulled outwards such that the electric current in the circuit changes at the rate of 8 A/s. At an instant when R is 12 Ω, the value of the current in the circuit will be A.
State Kirchhoff's law related to electrical circuits. In the given metre bridge, balance point is obtained at D. On connecting a resistance of 12 ohm parallel to S, balance point shifts to D'. Find the values of resistances R and S.