In a series R–L circuit, the voltage of the battery is \(10\ \text{V}\).
Resistance and inductance are \(10\ \Omega\) and \(10\ \text{mH}\) respectively.
Find the energy stored in the inductor when the current reaches \(\dfrac{1}{e}\) times its maximum value.
Show Hint
In R–L circuits, the maximum current is always \( \dfrac{V}{R} \).
Energy stored in an inductor depends only on the \textbf{instantaneous current}, not directly on time.
Concept:
For a series R–L circuit connected to a DC source:
The steady-state (maximum) current is given by \( I_{\max} = \dfrac{V}{R} \)
The energy stored in an inductor is given by \( U = \dfrac{1}{2} L I^2 \)
Step 1: Calculate the maximum current in the circuit.
\[
I_{\max} = \frac{V}{R} = \frac{10}{10} = 1\ \text{A}
\]
Step 2: Determine the current at the specified instant.
\[
I = \frac{1}{e} I_{\max} = \frac{1}{e}\ \text{A}
\]
Step 3: Write the formula for the energy stored in the inductor.
\[
U = \frac{1}{2} L I^2
\]
Given:
\[
L = 10\ \text{mH} = 0.01\ \text{H}
\]
Substituting values:
\[
U = \frac{1}{2} \times 0.01 \times \left(\frac{1}{e}\right)^2
\]
Step 4: Evaluate the expression.
\[
U = 0.005 \times \frac{1}{e^2}
\approx 0.005 \times 0.135
= 6.75 \times 10^{-4}\ \text{J}
\]
\[
U \approx 0.675\ \text{mJ}
\]
\[
U \approx 0.67\ \text{mJ}
\]