We know the emf induced in an inductor is given by: \[ \mathcal{E} = L \frac{dI}{dt} \] where \( L \) is the inductance of the inductor, \( I \) is the current, and \( \frac{dI}{dt} \) is the rate of change of current. The current increases uniformly from 0 to 2 A in 40 seconds, so the rate of change of current is: \[ \frac{dI}{dt} = \frac{2 \, \text{A}}{40 \, \text{s}} = 0.05 \, \text{A/s} \] Substituting this into the equation for emf: \[ \mathcal{E} = L \times 0.05 \] Given that the induced emf is 5 mV or \( 5 \times 10^{-3} \, \text{V} \), we can solve for \( L \): \[ 5 \times 10^{-3} = L \times 0.05 \] \[ L = \frac{5 \times 10^{-3}}{0.05} = 10^{-1} \, \text{H} = 0.1 \, \text{H} \] Now, the flux \( \Phi \) linked with the inductor at any time \( t \) is given by: \[ \Phi = L \times I \] At \( t = 10 \) s, the current is: \[ I = \frac{2 \, \text{A}}{40 \, \text{s}} \times 10 \, \text{s} = 0.5 \, \text{A} \] Thus, the flux at \( t = 10 \, \text{s} \) is: \[ \Phi = 0.1 \times 0.5 = 0.05 \, \text{Wb} \]

A coil of area A and N turns is rotating with angular velocity \( \omega\) in a uniform magnetic field \(\vec{B}\) about an axis perpendicular to \( \vec{B}\) Magnetic flux \(\varphi \text{ and induced emf } \varepsilon \text{ across it, at an instant when } \vec{B} \text{ is parallel to the plane of the coil, are:}\)
