Interactions generically have important effects on the topological quantum phases. For a quantum anomalous Hall (QAH) insulator, the presence of interactions can qualitatively change the topological phase diagram which, however, is typically hard to measure in the experiment. Here we propose a novel scheme based on quench dynamics to detect the mean-field topological phase diagram of an interacting Chern insulator, with nontrivial dynamical quantum physics being uncovered. We focus on a two-dimensional QAH system in the presence of a weak to intermediate Hubbard interaction which mainly induces a ferromagnetic order under the mean-field level. After quenching the Zeeman coupling, both the mean-field Hamiltonian and many-body quantum state evolve over time. This is in sharp contrast to quenching a non-interacting system, in which only the many-body state evolves. We find two characteristic times ts and tc which capture the emergence of dynamical self-consistent particle number density and dynamical topological phase transition for the time-dependent Hamiltonian, respectively. An interesting result is that ts > tc (ts < tc) occurs in repulsive (attractive) interaction when the system is quenched from an initial fully polarized state to the topologically nontrivial regimes, and ts = tc characterizes the topological phase boundaries. Moreover, the topological number of mean-field topological phase is determined by the spin polarizations of four Dirac points at the time ts. With these results we provide a feasible scheme to detect the mean-field topological phase diagram via the two characteristic times in quench dynamics, which can reveal the novel interacting effects on the topological phases and shall promote the experimental observation.