The dynamical evolution of a recently introduced one dimensional model in \cite{biswas-sen} (henceforth referred to as model I), has been made stochastic by introducing a parameter such that corresponds to the Ising model and to the original model I. The equilibrium behaviour for any value of is identical: a homogeneous state. We argue, from the behaviour of the dynamical exponent ,that for any $\beta \neq 0$, the system belongs to the dynamical class of model I indicating a dynamic phase transition at . On the other hand, the persistence probabilities in a system of spins saturate at a value $P_{sat}(\beta, L) = (\beta/L)^{\alpha}f(\beta)\alpha\beta \neq 0\beta =0$. The scaling function shows a crossover behaviour with $f(\beta) = \rm{constant} \beta <<1f(\beta) \propto \beta^{-\alpha}\beta >>1$.

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