Table 1.

Entropic representation of the thermodynamic fluxes and forces of Fourier–Navier–Stokes–Cahn–Hilliard–Korteweg fluids.

	thermal	diffusive	mechanical
fluxes	qi	ji	Pij − pδij − Zi∂j c
forces	${\mathrm{\partial }}_i({\displaystyle \frac{1}{T}})$	$-{\mathrm{\partial }}_i({\displaystyle \frac{\mu }{T}}-{\displaystyle \frac{1}{\rho }}{\mathrm{\partial }}_k({\displaystyle \frac{Z^k}{T}}))$	$-{\displaystyle \frac{{\mathrm{\partial }}_i{v}_j}{T}}$