First, we calculate the equivalent resistance \( R_{eq} \) of the circuit.
The two branches with \( 2 \, \Omega \) resistors are in parallel. The equivalent resistance for each pair of resistors in parallel is:
\[ \frac{1}{R_{eq}} = \frac{1}{2} + \frac{1}{2} = 1 \, \Omega. \]Since there are two such parallel branches in series, the total resistance \( R_{eq} \) of the circuit is:
\[ R_{eq} = 1 + 1 + \frac{2}{3} = \frac{4}{3} \, \Omega. \]The power \( P \) consumed in the circuit is given by:
\[ P = \frac{V^2}{R_{eq}}. \]Substitute \( V = 2 \, V \) and \( R_{eq} = \frac{4}{3} \, \Omega \):
\[ P = \frac{2^2}{\frac{4}{3}} = \frac{4}{\frac{4}{3}} = 3 \, W. \]Thus, the power consumption in the entire circuit is:
\[ 3 \, W. \]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: