The equations describe the induced electromotive force (emf) in a circuit:
\[ |e| = L \frac{dI}{dt} \]
The magnitude of the emf (\(|e|\)) is given by the product of inductance (\(L\)) and the rate of change of current (\(\frac{dI}{dt}\)).
\[ |e| = 6 \times 10^{-3} \left[ \frac{I_2 - I_1}{t_2 - t_1} \right] \]
Substituting the values, the emf is calculated using the discrete current change over time.
\[ |e| = 6 \times 10^{-3} \left[ \frac{1}{40 - 20} \right] \]
Plugging in the specific time interval (\(t_1 = 20\), \(t_2 = 40\)) and assuming the current change (\(\Delta I = 1\)).
\[ e = 3 \times 10^{-4} \text{ V} \]
The final result for the induced emf is \(3 \times 10^{-4}\) volts.