“…Under these concerns, the governing flow problem of 3D Carreau liquid is [17,45]. In overhead equations, (u, v, w) are the components of velocity along x-, y-and z-directions, respectively, n the power law exponent, the material rate constant, f , c f the specific heat and density of the Carreau liquid, the kinematic viscosity, (T, C) the liquid temperature and concentration of Carreau liquid, ( , * ), respectively, the relaxation time of heat and mass fluxes, D the molecular diffusivity of the concentration and K(T) the temperature-dependent thermal conductivity of Carreau liquid which is expressed as [49][50][51].…”