The induced emf \( \mathcal{E} \) in a coil is given by Faraday's law of induction:
\[
\mathcal{E} = - \frac{d\phi}{dt}
\]
where:
- \( \phi \) is the magnetic flux,
- \( \mathcal{E} \) is the induced emf.
Given:
\[
\phi = 5t^2 + 4t - 2
\]
Now, differentiate \( \phi \) with respect to time \( t \) to find the induced emf:
\[
\frac{d\phi}{dt} = \frac{d}{dt} \left( 5t^2 + 4t - 2 \right) = 10t + 4
\]
Thus, the induced emf is:
\[
\mathcal{E} = -(10t + 4)
\]
At \( t = 1 \) s:
\[
\mathcal{E} = -(10(1) + 4) = -(10 + 4) = -14 \ \text{V}
\]
The induced current \( I \) is given by Ohm's law:
\[
I = \frac{\mathcal{E}}{R}
\]
where:
- \( R = 14 \ \Omega \) is the resistance.
Substitute the values:
\[
I = \frac{-14}{14} = -1 \ \text{A}
\]
The magnitude of the induced current is:
\[
\boxed{1.0 \ \text{A}}
\]