Many technological devices used to intensify heat and mass transfer in a liquid or to spray it [i-8] are based on the phenomenon of motion of thin films in a field of centrifugal forces. In particular, when a glass-forming material is melted in a rotated plasmachemical reactor for producing mineral fiber, the molten mass moves over the inner surface of the device [8]. The properties of the material of the fibers produced are formed directly in the film moving under thermal and dynamic loading. Knowledge of the liquid-film thickness and its distribution along the axial coordinate in motion over the inner surface of a rotating cylinder allows one to calculate the heat exchange of such a film device.For an inner rotating cylindrical surface, Gol'dshtik [1] developed a theory of centrifugal sprayers, based on a model of potential motion of an inviscid liquid. However, comparison of the theoretical dependences obtained was performed with experimental results of studies of liquid-film spreading over a horizontal surface under gravity only. For viscous flows over an inner rotating cylindrical surface, there have been few experimental studies, and they poorly agree with theoretical studies. Leppert and Nimmo [3] calculated heat transfer for condensation of vapor on a liquid film moving down a horizontal plate. It is shown that even when the mass force is normal to the condensation surface, heat removal can have a finite value if running-off on the edges is allowed. In this case, the thickness of the condensate film and the resultant heat removal are controlled by varying the hydrostatic pressure across the film thickness. These results are applicable to condensation inside a rotating cylinder provided that the surface curvature is small and the rotational speed is high. However, to close a solution that describes this model, it is necessary to invoke two empirical parameters: the initial and final thicknesses of the condensate film. Postnikov [4] obtained a solution for the thickness of a laminar film moving over the inner surface of a rotating cylinder that requires one experimental value --the initial thickness of the film. Both solutions [3,4] have one feature in common: a sharp decrease to zero in the thickness of the moving liquid film, which is typical of a central flow region on the longitudinal coordinate.Early experimental studies in this field [5,6] were concerned with liquid flow in a rotating tube with broad rings at the edges. Dependences of the device capacity on the flow rate and angular frequency of rotation were obtained. Flow visualization using tracers in the form of a tinted liquid showed that the flow is of two-layer character. The main mass flow proceeded in a thin layer located closer to the center from the edge of the rings. The effect of viscosity on liquid flow in a rotating cylinder with various methods of feeding the liquid was studied experimentally in [7]. The results are somewhat unexpected: the thickness of the moving layer decreases with increase in viscosity. This effect was explained ...