The classical finite element method (FEM) fails to provide accurate results to the Helmholtz equation with large wave numbers due to the well-known "pollution error" caused by the numerical dispersion, i.e. the numerical wave number is always smaller than the exact one. This dispersion error is essentially rooted at the "overly-stiff" feature of the FEM model. In this paper, an alpha finite element method (α-FEM) is then formulated for the acoustic problems by combining the "smaller wave number" model of FEM and the "larger wave number" model of NS-FEM through a scaling factor a ∈ [0, 1]. The motivation for this combined approach is essentially from the features of "overly-stiff" FEM model and "overly-soft" NS-FEM model, and accurate solutions can be obtained by tuning the α-FEM model. A technique is proposed to determine a particular alpha with which the α-FEM model can possess a very "close-to-exact" stiffness, which can effectively reduce the dispersion error leading to dispersion free solutions for acoustic problems. Theoretical and numerical studies shall demonstrate the excellent properties of the present α-FEM.