The electromotive force (emf) induced in an inductor is defined by the equation: \[ \mathcal{E} = L \frac{dI}{dt} \] Here, \( L \) represents the inductance of the inductor, \( I \) denotes the current, and \( \frac{dI}{dt} \) signifies the rate of change of current. Given that the current rises linearly from 0 A to 2 A over a period of 40 seconds, the rate of current change is calculated as: \[ \frac{dI}{dt} = \frac{2 \, \text{A}}{40 \, \text{s}} = 0.05 \, \text{A/s} \] Substituting this value into the emf equation yields: \[ \mathcal{E} = L \times 0.05 \] With a known induced emf of 5 mV, equivalent to \( 5 \times 10^{-3} \, \text{V} \), we can determine the inductance \( L \): \[ 5 \times 10^{-3} = L \times 0.05 \] \[ L = \frac{5 \times 10^{-3}}{0.05} = 10^{-1} \, \text{H} = 0.1 \, \text{H} \] Subsequently, the magnetic flux \( \Phi \) linked with the inductor at any given time \( t \) is expressed as: \[ \Phi = L \times I \] At \( t = 10 \) seconds, the current is determined by: \[ I = \frac{2 \, \text{A}}{40 \, \text{s}} \times 10 \, \text{s} = 0.5 \, \text{A} \] Therefore, the flux at \( t = 10 \, \text{s} \) is: \[ \Phi = 0.1 \times 0.5 = 0.05 \, \text{Wb} \]