In this work, generalizing the techniques introduced by Jabir-Talay-Tomasevic [3], we prove the wellposedness and propagation of chaos for a stochastic particle system in mean-field interaction under the assumption that the interacting kernel belongs to a suitable $L^q_t −L^p_x$ space. Contrarty to the large deviation principle approach by [2], the main ingredient of the proof here are the partial Girsanov transformations introduced in [3].