In this paper, we study the influence of topological and noninertial effects on a Dirac particle confined in an Aharonov-Bohm (AB) ring. Next, we explicitly determine the Dirac spinor and the energy spectrum for the relativistic bound states. We observe that this spectrum depends on the quantum number n, magnetic flux Φ of the ring, angular velocity ω associated to the noninertial effects of a rotating frame, and on the deficit angle η associated to the topological effects of a cosmic string. We verified that this spectrum is a periodic function and grows in values as a function of n, Φ, ω, and η. In the nonrelativistic limit, we obtain the equation of motion for the particle, where now the topological effects are generated by a conic space. However, unlike relativistic case, the spectrum of this equation depends linearly on the velocity ω and decreases in values as a function of ω. Comparing our results with other works, we note that our problem generalizes some particular cases of the literature. For instance, in the absence of the topological and noninertial effects (η = 1 and ω = 0) we recover the usual spectrum of a particle confined in an AB ring (Φ = 0) or in an 1D quantum ring (Φ = 0).