Faraday's law of induction states that the induced electromotive force \( \mathcal{E} \) in a coil is \( \mathcal{E} = - \frac{d\phi}{dt} \), where \( \phi \) is the magnetic flux and \( \mathcal{E} \) is the induced emf.Given the magnetic flux \( \phi = 5t^2 + 4t - 2 \).Differentiating \( \phi \) with respect to time \( t \) yields \( \frac{d\phi}{dt} = \frac{d}{dt} \left( 5t^2 + 4t - 2 \right) = 10t + 4 \).Therefore, the induced emf is \( \mathcal{E} = -(10t + 4) \).At \( t = 1 \) s, the induced emf is \( \mathcal{E} = -(10(1) + 4) = -(10 + 4) = -14 \ \text{V} \).According to Ohm's law, the induced current \( I \) is \( I = \frac{\mathcal{E}}{R} \), where the resistance \( R = 14 \ \Omega \).Substituting the values, the induced current is \( I = \frac{-14}{14} = -1 \ \text{A} \).The magnitude of the induced current is \( \boxed{1.0 \ \text{A}} \).