“…In this illustration, the multiphases include water, heat, and chemicals. When a water pressure gradient ( grad p ), a chemical mass fraction gradient ( grad c ), and a temperature gradient ( grad T ) are applied across the mixture in a porous medium, the following situations are involved: (1) The pressure gradient causes the water molecules to migrate (usually from high pressure to lower pressure) with a mass flux of u = − ( k / v ) grad p , in which k is the permeability of the porous medium, v is the viscosity of the fluid, and u is the Darcy flux; (2) This water flow will be affected simultaneously by the chemical ( J = ρ f D grad c , where ρ f is the fluid mass density, D is the diffusion coefficient, and J is the diffusion flux) and thermal ( , in which λ is the thermal conduction coefficient and is the thermal flux) transport flows, and vice versa; (3) The secondary or tertiary coupled driving force may become the major driving force of the flow in some circumstances (eg, grad c becomes the major driving force of water flow rather than grad p for chemical osmosis in a membrane porous medium); (4) Overall, the 3 flows (water, chemical, and thermal) and 3 driving forces ( grad p , grad c , and grad T ) present a 3 × 3 matrix describing the cross‐couplings between each other (Figure ), which is the realistic condition of the multiphase porous medium system. Extensive experiments have been conducted in recent decades, but little has been achieved regarding theoretical development in a strict mathematical way.…”