Using first-principles calculations, we investigate the impact of hydrogenation on the Dzyaloshinskii-Moriya interaction (DMI) at graphene/Co interface. We find that both the magnitude and chirality of DMI can be controlled via hydrogenation absorbed on graphene surface. Our analysis using density of states combined with first-order perturbation theory reveals that the spin splitting and the occupation of Co-d orbitals, especially the and states, play a crucial role in defining the magnitude and the chirality of DMI. Moreover, we find that the DMI oscillates with a period of two atomic layers as a function of Co thickness what could be explained by analysis of out-of-plane of Co orbitals. Our work elucidates the underlying mechanisms of interfacial DMI origin and provides an alternative route of its control for spintronic applications.Topological magnetic textures, such as magnetic skyrmions [1-6] and chiral domain walls [7,8] can be used as information carriers for next generation information storage and logic technologies thanks to their high stability, small size and fast current driven mobility [9]. The Dzyaloshinskii-Moriya interaction (DMI) [10,11], which originates from spin-orbit coupling (SOC) in inversion symmetry broken system, plays a crucial role in the formation of these topological magnetic textures. Specifically, it can influence the chirality as well as stability and migration velocity of chiral domain walls and skyrmions [6,7]. Therefore, finding an efficient approach to control the magnitude and chirality of DMI is beneficial for creation and manipulation these magnetic textures for graphene spintronic applications.Recent reports indicate that the DMI can be induced at graphene/ferromagnetic metal interface [12,13].