The induced electromotive force (emf) \( \varepsilon \) in an inductor is given by Faraday's law of induction, which states that the induced emf is proportional to the rate of change of current through the inductor:
$$ \varepsilon = -L \frac{dI}{dt} $$
where \( L \) is the inductance of the inductor and \( \frac{dI}{dt} \) is the rate of change of current.
The negative sign indicates the direction of the induced emf (Lenz's law), but we are interested in the magnitude here.
Given:
Initial current \( I_1 = 2 \) A
Final current \( I_2 = 6 \) A
Time interval \( \Delta t = 2 \) s
Induced emf \( |\varepsilon| = 3 \) V
The change in current is \( \Delta I = I_2 - I_1 = 6 - 2 = 4 \) A.
The rate of change of current is \( \frac{dI}{dt} \approx \frac{\Delta I}{\Delta t} = \frac{4 \text{ A}}{2 \text{ s}} = 2 \text{ As}^{-1} \).
Now, we can find the inductance \( L \) using the magnitude of the induced emf:
$$ |\varepsilon| = L \left| \frac{dI}{dt} \right| $$
$$ 3 \text{ V} = L (2 \text{ As}^{-1}) $$
$$ L = \frac{3 \text{ V}}{2 \text{ As}^{-1}} = 1.
5 \text{ VsA}^{-1} $$
The unit of inductance is Henry (H), and 1 H = 1 VsA\(^{-1} \).
Therefore, the inductance of the inductor is \( L = 1.
5 \) H.