The influence of liquid mixing on mean logarithmic and arithmetic forces as well as the numbers of transfer units in direct flow has been studied. The extreme cases where liquid on the plate is entirely mixed and where it moves in a regime of perfect displacement are considered. The interrelationship between the mean arithmetic forces and numbers of transfer units in the case of complete liquid mixing and without it has been found. Dependences of the efficiency on the numbers of transfer units are determined.The effectiveness of mass transfer in direct motion of interacting flows is independent of liquid mixing on the tray. This characteristic feature of the direct flow is predetermined by the conditions of equilibrium between the vapor and liquid leaving the ideal plate and is observed in a complex model [1] and variants of mass transfer [2] with conditions of the relationship between an ideal plate and a real one that are typical of the models of Murphree and Hausen. In the most widespread models of Murphree [3][4][5] and Hausen [4][5][6], only complete mixing of liquid is foreseen. The computational relations, in particular, the effectiveness of mass transfer, are identical in the variants of mass transfer without mixing and in the above-mentioned models.At the same time, mixing of liquid exerts its influence on the magnitude of the motive forces. A liquid flow of composition x n arriving at the plate mixes up with the liquid present there and partially mixed and its concentration is decreased to x in (see Fig. 1). As a result of interaction with the vapor, the liquid is depleted of the highly volatile component and leaves the contact stage with the concentration x n−1 .In [7,8], with countercurrent and crosscurrent motion of phases, the mixing of the liquid is taken into account by the amount of completely mixed liquid ϕ. The other part of the liquid (1 − ϕ) moves on the plate in the regime of perfect displacement. Thus, the quantity ϕ characterizes the degree of liquid mixing. We will extend this expression to a direct flow. According to the assumption made, the composition of the liquid that arrives at the plate is expressed asand of that leaving the plate asIn a complex model with a direct flow [1], the initial composition of the arriving liquid, subject to formula (25) of [9], is equal toand the concentration of the escaping vapor, subject to the material balance equation L(x n − x n−1 ) = V(y n − y n−1 ), is