“…The latter approach includes the α-transformation of O'Rourke and Bracco [7], the pressure gradient scaling (PGS) method of Ramshaw et al [8], the acoustic speed reduction (ASR) method of Wang and Trouvé [9], the kinetically reduced local Navier-Stokes (KRLNS) equations of Ansumali et al [10] and Karlin et al [11], the artificial acoustic stiffness reduction method (AASCM) of Salinas-Vázquez et al [12], the entropically damped artificial compressibility (EDAC) method of Clausen [13] and the general pressure (GP) equation of Toutant [14]. These methods provide successive improvements to the numerical simulation of incompressible flows using artificial pressure equations and have been validated extensively for both laminar and turbulent viscous flows in the literature [11,15,13,16,17,18]. To the best knowledge of the authors, low Mach number flows with large temperature variations have been to date relatively ignored by these developments despite their ubiquitousness in a large variety of industrial applications, including heat exchangers, propulsion systems or nuclear or concentrated solar power plants [19,20,21,22].…”