Given the electric field of the electromagnetic wave:
\[ \vec{E} = \hat{i} 40 \cos \omega \left( t - \frac{z}{c} \right) \, \text{NC}^{-1} \]
In an electromagnetic wave, the magnetic field \(\vec{B}\) is perpendicular to both the electric field \(\vec{E}\) and the direction of propagation.
Since \(\vec{E}\) is along the \(\hat{i}\)-direction and the wave propagates along the \(\hat{k}\)-direction, the magnetic field \(\vec{B}\) must be along the \(\hat{j}\)-direction.
The relationship between the magnitudes of the electric and magnetic fields in an electromagnetic wave is given by:
\[ B = \frac{E}{c} \]
Substituting the given electric field magnitude:
\[ B = \frac{40}{c} \cos \omega \left( t - \frac{z}{c} \right) \]
Thus, the magnetic field is:
\[ \vec{B} = \hat{j} \frac{40}{c} \cos \omega \left( t - \frac{z}{c} \right) \]
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: