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: \[ \Phi = 0.1 \times 0.5 = 0.05 \, \text{Wb} \]
An ideal transformer is designed to convert 50 V into 250 V. It draws 200 W power from an AC source whose instantaneous voltage is given by \( v_i = 20 \sin(100\pi t) \, \text{V} \).
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