The power dissipated in the loop can be calculated using the formula:
\[ P = I^2 R \]
Where \(I\) is the induced current and \(R\) is the resistance.
The magnetic flux change through the loop is given by:
\[ \frac{dB}{dt} = 10^{-7} \, \text{T/s} \]
Using Faraday’s Law, the induced emf in the loop is:
\[ \mathcal{E} = -N \frac{d\Phi}{dt} \]
Now, calculate the induced current \(I\):
\[ I = \frac{\mathcal{E}}{R} \]
Substituting the values, we find the power dissipated:
\[ P = 2.16 \times 10^{-9} \, \text{W} \]
\[ P = 216 \times 10^{-9} \, \text{W} \]
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: