The induced emf (\( \mathcal{E} \)) in the coil is given by Faraday's law of induction, which states that:
\[
\mathcal{E} = - \frac{d\phi}{dt}
\]
where \( \phi \) is the magnetic flux. Substituting the given expression for \( \phi \), we first find the derivative of \( \phi \) with respect to time \( t \).
The given flux is:
\[
\phi = 2.0 t^3 + 5.0 t^2 + 6.0 t \, mWb}
\]
Now, differentiate \( \phi \) with respect to \( t \):
\[
\frac{d\phi}{dt} = 3 \times 2.0 t^2 + 2 \times 5.0 t + 6.0 = 6.0 t^2 + 10.0 t + 6.0
\]
At \( t = 2 \, s} \), substitute the value of \( t \) into the derivative:
\[
\frac{d\phi}{dt} = 6.0 \times (2)^2 + 10.0 \times (2) + 6.0 = 6.0 \times 4 + 10.0 \times 2 + 6.0 = 24 + 20 + 6 = 50.0 \, mWb/s}
\]
Thus, the induced emf is:
\[
\mathcal{E} = - 50.0 \, mV}
\]
Now, using Ohm's law, the induced current \( I \) through the coil is given by:
\[
I = \frac{\mathcal{E}}{R}
\]
where \( R = 5 \, \Omega \) is the resistance of the coil. Substituting the values:
\[
I = \frac{50.0 \times 10^{-3}}{5.0} = 10.0 \times 10^{-3} = 0.01 \, A} = 10 \, mA}
\]
Thus, the magnitude of the induced current at \( t = 2 \, s} \) is \( 10 \, mA} \).