A new model of chemical vapour transport constructed exclusively on the basis of thermodynamic quantities is presented. The transport process is considered as a series of consecutive cycles consisting of four following stages: (I) volatilization of the solid(s) in the dissolution zone; (II) migration of the vapour solution to the crystallization zone; (III) deposition of the solid(s) in the crystallization zone; (IV) migration of the vapour solution to the dissolution to the dissolution zone. In stage I, equilibrium exists between solid and gas phase. If the solid volatilizes incongruently, another solid has to appear, and therefore equilibrium between the two solids and the gas phase is established. In stage II, because of temperature change, homogeneous reactions (association, dissociation, etc.) proceed in the vapour. Owing to the reactions, the composition of the gas changes and a new equilibrium state is established between gaseous substances. Since no solids participate in these reactions, the vapour can become a supersaturated vapour solution. The solution can be in labile ot metastable state of equilibrium with some solid which can exist in considered system, but which may not necessarily be the solid (or one of two solids) existing in the dissolution zone. In stage III the solid to be deposited is the one remaining in the labile equilibrium state with the gas phase of the composition established after its arrival into the crystallization zone. In such a case, the supersaturation of the gas phase with regard to the solid to be deposited is higher than the so-called critical supersaturation. The deposition of the first solid causes subsequent changes in the gas phase composition. Thety can shift the labile vapour solution into the region in which another solid is deposited as the next one if the supersaturation of the gas phase with regard to the solid is higher than the critical one, and so on. The deposition proceeds until the equilibrium between the deposited solid and the gas phase is established. If the superstation is lower than the critical one, the deposition of the solid cannot proceed and the gas phase remains a supersaturated metastable vapour solution. Considering the gas phase composition changes in the successive stages of the cycle, one can explain the behaviour of the transport system or determine the preconditions for depositing a solid of desirable composition.