METHOD FOR DETERMINING THE RATE thermocapillary flow in side surface SHAYBOVIDNOGO BUBBLE

摘要

method u043eu043fu0440u0435u0434u0435u043bu0435u043du0438u00a0 speed u0442u0435u0440u043cu043eu043au0430u043fu0438u043bu043bu00a0u0440u043du043eu0433u043e u0442u0435u0447u0435u043du0438u00a0 at the lateral surface of the u0448u0430u0439u0431u043eu0432u0438u0434u043du043eu0433u043e vials, u043eu0442u043bu0438u0447u0430u044eu0449u0438u0439u0441u00a0, u0442u0435u0440u043cu043eu043au0430u043fu0438u043bu043bu00a0u0440u043du043eu0435 for u0432u043eu0437u0431u0443u0436u0434u0430u0435u0442u0441u00a0 pooch one of the light, and the speed of u043au0430u043fu0438u043bu043bu00a0u0440u043du043eu0433u043e u043eu043fu0440u0435u0434u0435u043bu00a0u0435u0442u0441u00a0 balance and dynamic pressures acting on the side surface of the bottle, as caused by the u0442u0435u0440u043cu043eu043au0430u043fu0438 u043bu043bu00a0u0440u043du044bu043c over its dynamic deformation, curvature,according to the principle of superposition, u0441u043au043bu0430u0434u044bu0432u0430u0435u0442u0441u00a0 with static camber that the total curvature of the deformed u043fu043eu0432u0435u0440u0445u043d u0434u0430u0432u0430u00a0 observed visually guests u043eu043fu0440u0435u0434u0435u043bu00a0u0435u043cu043eu0439 by u0438u0437u043cu0435u0440u0435u043du0438u00a0 bottle and its radius of curvature.