To determine the electromotive force (emf) induced in the coil, we will use Faraday's Law of Electromagnetic Induction, which states that the induced emf in a coil is given by the rate of change of the magnetic flux through the coil. The formula for emf (\( \mathcal{E} \)) is:
\mathcal{E} = -N \frac{\Delta \Phi}{\Delta t}
Where:
The magnetic flux (\( \Phi \)) through a single turn of the coil is given by:
\Phi = B \cdot A \cdot \cos(\theta)
Where:
Initially, the coil is perpendicular to the magnetic field, so \theta = 0^\circ, and thus:
\Phi_{\text{initial}} = 5 \times 10^{-5} \cdot 0.05 \cdot \cos(0^\circ) = 2.5 \times 10^{-6} \, \text{Wb}
After rotating the coil by \(90^\circ\), the angle becomes \(90^\circ\), and the new magnetic flux is:
\Phi_{\text{final}} = 5 \times 10^{-5} \cdot 0.05 \cdot \cos(90^\circ) = 0 \, \text{Wb}
The change in magnetic flux (\( \Delta \Phi \)) is:
\Delta \Phi = \Phi_{\text{final}} - \Phi_{\text{initial}} = 0 - 2.5 \times 10^{-6} = -2.5 \times 10^{-6} \, \text{Wb}
Substituting the values into Faraday's law, we have:
\mathcal{E} = -800 \cdot \frac{-2.5 \times 10^{-6}}{0.1} = 800 \cdot 2.5 \times 10^{-5} = 0.02 \, \text{V}
Therefore, the induced emf in the coil is 0.02 V.