At steady state, the inductor behaves as a short circuit, meaning it has zero resistance. The circuit becomes a simple resistor connected to the voltage source.
Using Ohm’s law, the steady-state current (\( I \)) through the resistor is given by:
\[ I = \frac{V}{R}. \]
Substitute \( V = 10 \, \text{V} \) and \( R = 4 \, \Omega \):
\[ I = \frac{10}{4} = \frac{5}{2} = 2.5 \, \text{A}. \]
The energy (\( E \)) stored in the magnetic field of the inductor is given by:
\[ E = \frac{1}{2} L I^2. \]
Substitute \( L = 2 \, \text{H} \) and \( I = 2.5 \, \text{A} \):
\[ E = \frac{1}{2} \cdot 2 \cdot \left(2.5\right)^2. \]
Calculate \( (2.5)^2 \):
\[ (2.5)^2 = 6.25. \]
Substitute back into the equation:
\[ E = \frac{1}{2} \cdot 2 \cdot 6.25 = 6.25 \, \text{J}. \]
Convert to scientific notation:
\[ E = 625 \times 10^{-2} \, \text{J}. \]
The energy stored in the magnetic field is \( 625 \times 10^{-2} \, \text{J} \).
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: