The induced emf \( \varepsilon \) is given by Faraday’s law of induction:
\[
\varepsilon = -N \frac{d\phi}{dt}.
\]
Here, \( N \) is the number of turns in the coil, and \( \phi \) is the magnetic flux. The flux is related to the magnetic field \( B \) and the area \( A \) of the coil.
The magnetic flux changes due to the change in current in the solenoid, causing an induced emf. The induced emf is:
\[
\varepsilon = -N \mu_0 n \pi r^2 \frac{dI}{dt}.
\]
Given values:
\( N = 100 \),
\( n = 250 \, \text{turns/cm} \),
\( r = 1.6 \, \text{cm} \),
\( dI = 1.5 \, \text{A} \),
\( dt = 25 \, \text{ms} \).
Substituting the values:
\[
\varepsilon = 0.1536 \, \text{V}.
\]
The current induced in the coil is:
\[
I = \frac{\varepsilon}{R} = \frac{0.1536}{5} = 0.03 \, \text{A}.
\]