The heat passing through the cross-section of a conductor, varies with time ‘t’ as Q(t) = αt – βt2 + γt3. (α, β and γ are positive constants.) The minimum heat current through the conductor is
(1) \(\alpha - \frac{\beta^2}{2\gamma}\)
(2) \(\alpha - \frac{\beta^2}{3\gamma}\)
(3) \(\alpha - \frac{\beta^2}{\gamma}\)
(4) \(\alpha - \frac{3\beta^2}{\gamma}\)