In this paper, by establishing a Brans-Dicke (BD) cosmology by means of a deformed phase space, in the absence of any scalar potential, cosmological constant and ordinary matter, we show that it is feasible to overcome obstacles reported in the corresponding commutative (nondeformed) frameworks. More concretely, by applying the Hamiltonian formalism and introducing a dynamical deformation, between the momenta associated to the FLRW scale factor and the BD scalar field, we obtain the modified equations of motion. In particular, these equations reduce to their standard counterparts when the noncommutative (NC) parameter is switched off. By focusing on a specific branch of solutions, in contrast to standard frameworks (even with a varying BD coupling parameter), we show that we can obtain an adequate appropriate inflationary epoch possessing a suitable graceful exit. In other words, in the Jordan frame (JF), such branch of solutions properly satisfy the sufficient condition required for satisfactory inflation, which is equivalent to get an inflationary phase in the conformal Einstein frame (EF) without branch change. Concerning the cosmological dynamics, we further show that our NC framework bears close resemblance to the R 2 (Starobinsky) inflationary model. 1 Recently, concerning such an ad hoc scalar potential in scalar tensor theories, it has been shown that the geometry of the higher dimensions can instead naturally yield it; see, for instance, [9,10,11,12]. Moreover, we should note that, in addition to including a scalar potential, there are also other approaches for describing the present day acceleration (which, in turn, suffer from major problems [13]): (i) When the BD coupling parameter is restricted to −2 ≤ ω ≤ −3/2; in this case, the energy condition associated to the BD scalar field is not satisfied. In this paper, to avoid encountering such a problem, we always assume −3/2 < ω. (ii) Assuming a varying BD coupling parameter [14]. (iii) Assuming that the scalar fields can interact with ordinary matter, which are called chameleon fields [15]. (iv) By starting from the BD theory in five or higher dimensional space-times, see for instance, [16]. We should emphasize that the motivation of