24 research outputs found

    Control of flow structure inside semi-cylindrical trench

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    Π— ΠΌΠ΅Ρ‚ΠΎΡŽ ΠΏΠΎΡˆΡƒΠΊΡƒ способів кСрування ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½ΠΈΠΌΠΈ Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΠΌΠΈ структурами Π² ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΈΡ… ΡˆΠ°Ρ€Π°Ρ… Π² Π°Π΅Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½Ρ–ΠΉ Ρ‚Ρ€ΡƒΠ±Ρ– Π²Ρ–Π΄ΠΊΡ€ΠΈΡ‚ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΡƒ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π΅ дослідТСння Ρ‚Π΅Ρ‡Ρ–Ρ— усСрСдині заглиблСння Π½Π° плоскій ΠΎΠ±Ρ‚Ρ–Ρ‡Π½Ρ–ΠΉ ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ– Π· використанням Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π° Ρ‚Π° ΠΏΠΎΡ€ΠΎΡˆΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρƒ Π²Ρ–Π·ΡƒΠ°Π»Ρ–Π·Π°Ρ†Ρ–Ρ—. ДослідТСння Π²ΠΈΠΊΠΎΠ½Π°Π½ΠΎ ΠΏΡ€ΠΈ ΠΎΠ±Ρ‚Ρ–ΠΊΠ°Π½Π½Ρ– ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡ–Π²Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΎΠ³ΠΎ заглиблСння (Π· Π²Ρ–Π΄Π½ΠΎΡˆΠ΅Π½Π½ΡΠΌ Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€Π° Π΄ΠΎ Π΄ΠΎΠ²ΠΆΠΈΠ½ΠΈ 0.23) ΠΏΡ€ΠΈ відсутності Ρ‚Π° наявності ΠΊΠ΅Ρ€ΡƒΠ²Π°Π»ΡŒΠ½ΠΈΡ… Π΄Ρ–ΠΉ Π²Ρ–Π΄ встановлСння Ρ€Ρ–Π·Π½ΠΎΠΌΠ°Π½Ρ–Ρ‚Π½ΠΈΡ… ΠΊΠΎΠ·ΠΈΡ€ΠΊΡ–Π² Π½Π° ΠΏΠ΅Ρ€Π΅Π΄Π½Ρ–ΠΉ Π·Π° ΠΏΠΎΡ‚ΠΎΠΊΠΎΠΌ Ρ‚Π° ΠΊΠΎΡ€ΠΌΠΎΠ²Ρ–ΠΉ ΠΊΡ€ΠΎΠΌΠΊΠ°Ρ… заглиблСння. Досліди ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΏΡ€ΠΈ Π·Π½Π°Ρ‡Π΅Π½Π½Ρ– числа РСйнольдса ΠΏΠΎ Π΄ΠΎΠ²ΠΆΠΈΠ½Ρ– пластини (Π²Ρ–Π΄ Ρ—Ρ— ΠΏΠΎΡ‡Π°Ρ‚ΠΊΡƒ Π΄ΠΎ Ρ†Π΅Π½Ρ‚Ρ€Π° заглиблСння) 1.23Β·105. Показано, Ρ‰ΠΎ Π² залСТності Π²Ρ–Π΄ Ρ€ΠΎΠ·Ρ‚Π°ΡˆΡƒΠ²Π°Π½Π½Ρ ΠΊΠΎΠ·ΠΈΡ€ΠΊΡ–Π² ΠΌΠΎΠΆΠ½Π° суттєво Π²ΠΏΠ»ΠΈΠ²Π°Ρ‚ΠΈ Π½Π° Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΠΉ Ρ€ΡƒΡ… усСрСдині заглиблСння. ΠŸΡ€ΠΈ Π²ΠΈΠ±ΠΎΡ€Ρ– ΠΏΠ΅Π²Π½ΠΈΡ… ΠΊΠΎΠ½Ρ„Ρ–Π³ΡƒΡ€Π°Ρ†Ρ–ΠΉ ΠΊΠΎΠ·ΠΈΡ€ΠΊΡ–Π² Π΄ΠΎΡΡΠ³Π°ΡŽΡ‚ΡŒΡΡ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ– Π²ΠΈΠΏΠ°Π΄ΠΊΠΈ: Π°Π±ΠΎ ΠΏΠΎΠ²Π½Π° консСрвація ΠΏΠΎΡ€ΠΎΡˆΠΊΡƒ усСрСдині заглиблСння, Π°Π±ΠΎ, Π·Π° Π½Π΅ΠΎΠ±Ρ…Ρ–Π΄Π½Ρ–ΡΡ‚ΡŽ, ΠΏΠΎΠ²Π½Π΅ вимивання ΠΏΠΎΡ€ΠΎΡˆΠΊΡƒ Ρ–Π· заглиблСння. Π’Π°ΠΊΠΈΠΌ Ρ‡ΠΈΠ½ΠΎΠΌ, виявлСно ΠΌΠ΅Ρ…Π°Π½Ρ–Π·ΠΌΠΈ кСрування ΡΡ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€ΠΎΡŽ Ρ‚Π΅Ρ‡Ρ–Ρ— Π² Π·Π°Π³Π»ΠΈΠ±Π»Π΅Π½Π½Ρ–, Ρ‰ΠΎ Π²Ρ–Π΄ΠΊΡ€ΠΈΠ²Π°Ρ” пСрспСктиву управління процСсами тСпломасопСрСносу Π½Π° ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΈΡ… повСрхнях Ρ‚Π΅Ρ…Π½Ρ–Ρ‡Π½ΠΈΡ… пристроїв.The purpose of research is search and testing of new means of coherent vortical structures control in boundary layers, what can be used for control of heat and mass transfer processes. Experimental study of current inside semi-cylindrical trench on flat surface was carried out in the wind-channel of the opened type using thermoanemometer and powder-like method of visualization. Investigation was realized in semi-cylindrical cavity which was disposed across to undisturbed stream for the flow Reynolds number according to length of plate (from its beginning to the trench midpoint) 1.23Β·105. Ratio of cavity diameter to its length was 0.23. The coherent vortical structures inside of trench were discovered and investigated for cases of absence and existence of control actions by means of setting along the trench length of various screens on leading edge of cavity regarding to the incident flow and also on back edge of cavity. It is shown that depending from different location of screens it is possible to influence substantially on a vortex motion in cavity, and choice of certain configuration of controlling screens gives the possibility to obtain or the complete preservation of monodispersible powder in cavity, either, if is necessary, complete breaking out of powder from cavity. Thus applied control means allow to comprehend and to employ the mechanism of current structure control and accordingly heat and mass transfer processes on exposed surfaces of aircraft, cosmic, marine, power technique.Π‘ Ρ†Π΅Π»ΡŒΡŽ поиска способов управлСния ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½Ρ‹ΠΌΠΈ Π²ΠΈΡ…Ρ€Π΅Π²Ρ‹ΠΌΠΈ структурами Π² ΠΏΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… слоях Π² аэродинамичСской Ρ‚Ρ€ΡƒΠ±Π΅ ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ° ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ΅ исслСдованиС тСчСния Π² полости углублСния Π½Π° плоской ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π΅ΠΌΠΎΠΉ повСрхности с использованиСм Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π° ΠΈ ΠΏΠΎΡ€ΠΎΡˆΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π²ΠΈΠ·ΡƒΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ. ИсслСдованиС Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΠΏΡ€ΠΈ ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π½ΠΈΠΈ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ полуцилиндричСского углублСния (с ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠ΅ΠΌ Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€Π° ΠΊ Π΄Π»ΠΈΠ½Π΅ 0.23) ΠΏΡ€ΠΈ отсутствии ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ ΡƒΠΏΡ€Π°Π²Π»ΡΡŽΡ‰ΠΈΡ… воздСйствий ΠΎΡ‚ установки Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… ΠΊΠΎΠ·Ρ‹Ρ€ΡŒΠΊΠΎΠ² Π½Π° ΠΏΠ΅Ρ€Π΅Π΄Π½Π΅ΠΉ ΠΏΠΎ ΠΏΠΎΡ‚ΠΎΠΊΡƒ ΠΈ ΠΊΠΎΡ€ΠΌΠΎΠ²ΠΎΠΉ ΠΊΡ€ΠΎΠΌΠΊΠ°Ρ… углублСния. ΠžΠΏΡ‹Ρ‚Ρ‹ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ‹ ΠΏΡ€ΠΈ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΈ числа РСйнольдса ΠΏΠΎ Π΄Π»ΠΈΠ½Π΅ пластины (ΠΎΡ‚ Π΅Ρ‘ Π½Π°Ρ‡Π°Π»Π° Π΄ΠΎ Ρ†Π΅Π½Ρ‚Ρ€Π° углублСния) 1.23Β·105. Показано, Ρ‡Ρ‚ΠΎ Π² зависимости ΠΎΡ‚ располоТСния ΠΊΠΎΠ·Ρ‹Ρ€ΡŒΠΊΠΎΠ² ΠΌΠΎΠΆΠ½ΠΎ сущСствСнно Π²Π»ΠΈΡΡ‚ΡŒ Π½Π° Π²ΠΈΡ…Ρ€Π΅Π²ΠΎΠ΅ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π² ΡƒΠ³Π»ΡƒΠ±Π»Π΅Π½ΠΈΠΈ. ΠŸΡ€ΠΈ Π²Ρ‹Π±ΠΎΡ€Π΅ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Ρ‘Π½Π½Ρ‹Ρ… ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΉ ΠΊΠΎΠ·Ρ‹Ρ€ΡŒΠΊΠΎΠ² Π΄ΠΎΡΡ‚ΠΈΠ³Π°ΡŽΡ‚ΡΡ ΠΏΡ€Π΅Π΄Π΅Π»ΡŒΠ½Ρ‹Π΅ случаи: Π»ΠΈΠ±ΠΎ полная консСрвация ΠΏΠΎΡ€ΠΎΡˆΠΊΠ° Π² полости углублСния, Π»ΠΈΠ±ΠΎ, ΠΏΡ€ΠΈ нСобходимости, ΠΏΠΎΠ»Π½ΠΎΠ΅ Π²Ρ‹ΠΌΡ‹Π²Π°Π½ΠΈΠ΅ ΠΏΠΎΡ€ΠΎΡˆΠΊΠ° ΠΈΠ· углублСния. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ, выявлСны ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΡ‹ управлСния структурой тСчСния Π² ΡƒΠ³Π»ΡƒΠ±Π»Π΅Π½ΠΈΠΈ, Ρ‡Ρ‚ΠΎ ΠΎΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ пСрспСктиву управлСния процСссами тСпломассообмСна Π½Π° ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π΅ΠΌΡ‹Ρ… повСрхностях тСхничСских устройств

    Influence of semicylindrical cavity on integral characteristics of wall boundary layer

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    НавСдСно Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ– дослідТСння Π· вивчСння характСристик ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠ³ΠΎ ΡˆΠ°Ρ€Ρƒ Π½Π°Π΄ плоскою ΠΏΠ»Π°ΡΡ‚ΠΈΠ½ΠΎΡŽ Π· Π½Π°ΠΏΡ–Π²Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΎΡŽ канавкою, яка ΠΎΠ±Ρ‚Ρ–ΠΊΠ°Ρ”Ρ‚ΡŒΡΡ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΈΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠΎΠΌ. ВстановлСно, Ρ‰ΠΎ формування Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΠ³ΠΎ Ρ€ΡƒΡ…Ρƒ усСрСдині заглиблСння суттєво Π²ΠΏΠ»ΠΈΠ²Π°Ρ” Π½Π° ΠΏΡ€ΠΎΡ„Ρ–Π»Ρ– ΠΏΠΎΠ·Π΄ΠΎΠ²ΠΆΠ½ΡŒΠΎΡ— ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– Ρƒ ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠΌΡƒ ΡˆΠ°Ρ€Ρ–, Π½Π° Ρ‚ΠΎΠ²Ρ‰ΠΈΠ½Ρƒ витіснСння, Ρ‚ΠΎΠ²Ρ‰ΠΈΠ½Ρƒ Π²Ρ‚Ρ€Π°Ρ‚ΠΈ Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΡƒ Ρ‚Π° Ρ„ΠΎΡ€ΠΌΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€. ΠžΠ±Ρ€Π°Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° дослідТСння Ρ€ΠΎΠ±ΠΈΡ‚ΡŒ Π΄ΠΎΡΡ‚Π°Ρ‚Π½ΡŒΠΎ Ρ–Π½Ρ„ΠΎΡ€ΠΌΠ°Ρ‚ΠΈΠ²Π½ΠΈΠΌΠΈ Π΄Π°Π½Ρ–, Ρ‰ΠΎ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– використанням ΠΎΠ΄Π½ΠΎΠ½ΠΈΡ‚ΠΊΠΎΠ²ΠΎΠ³ΠΎ Π΄Π°Ρ‚Ρ‡ΠΈΠΊΠ° Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π°. ВиявлСний Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ Π·ΠΌΡ–Π½ Ρ–Π½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΈΡ… характСристик ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠ³ΠΎ ΡˆΠ°Ρ€Ρƒ ΠΏΠ΅Ρ€Π΅Π΄ заглиблСнням, Π½Π°Π΄ Π½ΠΈΠΌ Ρ‚Π° Π·Π° Π½ΠΈΠΌ Π²Ρ–Π΄ΠΎΠ±Ρ€Π°ΠΆΠ°Ρ” Π²ΠΏΠ»ΠΈΠ² дисипативних Ρ‚Π° Ρ–Π½Π΅Ρ€Ρ†Ρ–ΠΉΠ½ΠΈΡ… Π΅Ρ„Π΅ΠΊΡ‚Ρ–Π² Π½Π° структуру Ρ‚Π΅Ρ‡Ρ–Ρ— як ΡƒΠ²Π΅Ρ€Ρ… ΠΏΡ€ΠΎΡ‚ΠΈ ΠΏΠΎΡ‚ΠΎΠΊΡƒ, Ρ‚Π°ΠΊ Ρ– Π·Π° Π½ΠΈΠΌ, Π° Ρ‚Π°ΠΊΠΎΠΆ дозволяє Π²ΠΈΠ·Π½Π°Ρ‡ΠΈΡ‚ΠΈ Π·ΠΎΠ½ΠΈ Ρ€ΠΎΠ·Ρ‚Π°ΡˆΡƒΠ²Π°Π½Π½Ρ ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½ΠΈΡ… Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур Π² ΠΏΠΎΡ€ΠΎΠΆΠ½ΠΈΠ½Ρ– ΠΊΠ°Π½Π°Π²ΠΊΠΈ, ΠΎΡ†Ρ–Π½ΠΈΡ‚ΠΈ ΡƒΠΌΠΎΠ²ΠΈ Ρ‚Π°, частково, ΠΏΡ€ΠΈΡ€ΠΎΠ΄Ρƒ Ρ—Ρ… виникнСння.Process control of mass and heat transfer in liquid and gas flows by means of cavities at the streamlined surfaces is one of the most promising ways to save energy in industrial, transport and power units and machines. The cause of this experimental study setting was deficit of information about coherent vortex structures (CVS) formation and emission from the grooves in the wake flow. To obtain this information in this work we investigate the profiles of the defects of the longitudinal velocity, displacement thickness, momentum thickness and shape factor in the boundary layer of air flow in front, above and behind the surface semi-cylindrical indentation on a flat plate. Analysis of these data shows that they reflect the influence of dissipative and inertial effects on the structure of the flow and allow us to determine the location of the CVS zones in the cavity of the groove and to better understand the conditions and nature of their beginning. Quantitative and qualitative changes of shape factor along the longitudinal coordinate as a function of flow velocity are significantly differ from traditional notions about weak dependence of this characteristic from Reynolds number, that is peculiar to flow over the plates and wing profiles without indentations. The proposed organization and implementation of experiments allow to receive sufficiently effective data by using per single hot-wire sensor of thermoanemometer. Pictures of the formation and evolution of the CVS expend complementary to the boundary conditions database for numerical calculations of heat transfer and aerodynamic drag in the flow with small Mach numbers over surface indentations. Results of investigation may be useful in designing of surfaces for aircrafts, ships and ground transports, as well as efficient compact heat exchangers.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ исслСдования изучСния характСристик ΠΏΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½ΠΎΠ³ΠΎ слоя Π½Π°Π΄ плоской пластиной с полуцилиндричСской ΠΊΠ°Π½Π°Π²ΠΊΠΎΠΉ, ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π΅ΠΌΠΎΠΉ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½Ρ‹ΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠΎΠΌ. УстановлСно, Ρ‡Ρ‚ΠΎ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΈΡ…Ρ€Π΅Π²ΠΎΠ³ΠΎ двиТСния Π²Π½ΡƒΡ‚Ρ€ΠΈ углублСния сущСствСнно влияСт Π½Π° ΠΏΡ€ΠΎΡ„ΠΈΠ»ΠΈ Π΄Π΅Ρ„Π΅ΠΊΡ‚ΠΎΠ² ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠΉ скорости Π² ΠΏΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½ΠΎΠΌ слоС, Π½Π° Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Ρƒ вытСснСния, Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Ρƒ ΠΏΠΎΡ‚Π΅Ρ€ΠΈ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° ΠΈ Ρ„ΠΎΡ€ΠΌΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€. Выбранная ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° исслСдования Π΄Π΅Π»Π°Π΅Ρ‚ достаточно ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ‚ΠΈΠ²Π½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹Π΅, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ примСнСния ΠΎΠ΄Π½ΠΎΠ½ΠΈΡ‚ΠΎΡ‡Π½ΠΎΠ³ΠΎ Π΄Π°Ρ‚Ρ‡ΠΈΠΊΠ° Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π°. ΠžΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Π½Ρ‹ΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ измСнСния ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… характСристик ΠΏΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½ΠΎΠ³ΠΎ слоя ΠΏΠ΅Ρ€Π΅Π΄ ΡƒΠ³Π»ΡƒΠ±Π»Π΅Π½ΠΈΠ΅ΠΌ, Π½Π°Π΄ Π½ΠΈΠΌ ΠΈ Π·Π° Π½ΠΈΠΌ ΠΎΡ‚Ρ€Π°ΠΆΠ°Π΅Ρ‚ влияниС диссипативных ΠΈ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… эффСктов Π½Π° структуру тСчСния ΠΊΠ°ΠΊ Π²Π²Π΅Ρ€Ρ… ΠΏΡ€ΠΎΡ‚ΠΈΠ² ΠΏΠΎΡ‚ΠΎΠΊΠ°, Ρ‚Π°ΠΊ ΠΈ Π²Π½ΠΈΠ· ΠΏΠΎ ΠΏΠΎΡ‚ΠΎΠΊΡƒ, Π° Ρ‚Π°ΠΊΠΆΠ΅ позволяСт ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΡ‚ΡŒ Π·ΠΎΠ½Ρ‹ располоТСния ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½Ρ‹Ρ… Π²ΠΈΡ…Ρ€Π΅Π²Ρ‹Ρ… структур Π² полости ΠΊΠ°Π½Π°Π²ΠΊΠΈ, ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ условия ΠΈ, частично, ΠΏΡ€ΠΈΡ€ΠΎΠ΄Ρƒ ΠΈΡ… возникновСния

    Vorticity formation inside and near cross-streamlined semi-cylindrical trench on flat surface

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    Розглянуті особливості формування поля завихрСності усСрСдині Ρ‚Π° ΠΏΠΎΠ±Π»ΠΈΠ·Ρƒ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΎΡ— Π½Π°ΠΏΡ–Π²Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΎΡ— Ρ‚Ρ€Π°Π½ΡˆΠ΅Ρ— Π½Π° Π³Ρ–Π΄Ρ€Π°Π²Π»Ρ–Ρ‡Π½ΠΎ Π³Π»Π°Π΄ΠΊΡ–ΠΉ пласкій ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ–. НавСдСно Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΈΡ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ усСрСднСних Ρ– ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉΠ½ΠΈΡ… складових ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΡ— завихрСності, які ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΎ для Ρ€Ρ–Π·Π½ΠΈΡ… Ρ€Π΅ΠΆΠΈΠΌΡ–Π² Ρ‚Π΅Ρ‡Ρ–Ρ— Ρƒ Π°Π΅Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½Ρ–ΠΉ Ρ‚Ρ€ΡƒΠ±Ρ–. ДослідТСння проводилися Ρ–Π· застосуванням дротяного Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π°. Π—Π½Π°ΠΉΠ΄Π΅Π½ΠΎ, Ρ‰ΠΎ Π½Π°ΠΉΠ±Ρ–Π»ΡŒΡˆΡ– Ρ€Ρ–Π²Π½Ρ– осСрСднСної завихрСності ΡΠΏΠΎΡΡ‚Π΅Ρ€Ρ–Π³Π°ΡŽΡ‚ΡŒΡΡ ΠΏΠΎΠ±Π»ΠΈΠ·Ρƒ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΈΡ… ΠΏΠΎΠ²Π΅Ρ€Ρ…ΠΎΠ½ΡŒ Ρ– Π² ΠΊΡƒΡ‚ΠΎΠ²ΠΈΡ… областях Ρ‚Ρ€Π°Π½ΡˆΠ΅Ρ— – Ρ‚Π°ΠΌ, Π΄Π΅ Π²Ρ–Π΄Π±ΡƒΠ²Π°Ρ”Ρ‚ΡŒΡΡ Π²Ρ–Π΄Ρ€ΠΈΠ² ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠ³ΠΎ ΡˆΠ°Ρ€Ρƒ Ρ‚Π° взаємодія Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур ΡˆΠ°Ρ€Ρƒ Π·ΠΌΡ–ΡˆΡƒΠ²Π°Π½Π½Ρ Π· квазистійким Π²Π΅Π»ΠΈΠΊΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΈΠΌ Π²ΠΈΡ…ΠΎΡ€ΠΎΠΌ Ρ–, особливо, ΠΏΠΎΠ±Π»ΠΈΠ·Ρƒ ΠΊΠΎΡ€ΠΌΠΎΠ²ΠΎΡ— стінки.The article are devoted to elucidation of current macro- and microstructure inside of semi-cylindrical trench and near its in boundary layer on flat plate by means of investigation of vorticity distributions. Vorticity defines rotational components and physics of any liquid and gas motion, but in turbulent flows on working surfaces with geometric large-scale irregularities by indentations type and in currents with coherent vortical structures the vorticity takes the most important part in processes of mass, momentum and energy transfer. For better understanding of mechanism of indicated phenomenon this paper offers some new scientific results on experimental research of vorticity and its fluctuations fields in the region of the cross-streamlined semi-cylindrical trench on a flat surface for different flow regimes according to Reynolds numbers range (by trench diameter) Red = 1,48βˆ™10Β³ Γ· 2,68βˆ™10⁴. The experimental investigation was carried out on open-circuit wind tunnell equipped by constant temperature anemometer with hot-wire probes, laser instrumentation, vibration and acoustic analyzer. The measurements of local time-averaged velocities and velocity fluctuations discovered that the most levels of mean vorticity take place near by the streamlined surfaces and in the angular areas of trench where boundary layer is separated and vortex structures of the shear blending layer are interacted with back wall of the trench. Zones of increased voticity fluctuation levels are disposed mainly between maximum mean vorticity regions and in area formed by interaction of coherent vortical structures of shear blending layer with quasi-stable large-scale eddy generated owing to impact interaction of blending layer with trench back wall. Results of investigation may be used for efficiency estimations of transfer processes on streamlined elements of heat exchangers, engines, ships, aircrafts etc.РассмотрСны особСнности формирования поля завихрСнности Π²Π½ΡƒΡ‚Ρ€ΠΈ ΠΈ Π²Π±Π»ΠΈΠ·ΠΈ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π΅ΠΌΠΎΠΉ полуцилиндричСской Ρ‚Ρ€Π°Π½ΡˆΠ΅ΠΈ Π½Π° гидравличСски Π³Π»Π°Π΄ΠΊΠΎΠΉ плоской повСрхности. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… исслСдований осрСднСнных ΠΈ ΠΏΡƒΠ»ΡŒΡΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΡ… ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠΉ завихрСнности, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ для Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ€Π΅ΠΆΠΈΠΌΠΎΠ² тСчСния Π² аэродинамичСской Ρ‚Ρ€ΡƒΠ±Π΅. ИсслСдования ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡŒ с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΡ€ΠΎΠ²ΠΎΠ»ΠΎΡ‡Π½ΠΎΠ³ΠΎ Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Π°. ΠžΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ΠΎ, Ρ‡Ρ‚ΠΎ наибольшиС ΡƒΡ€ΠΎΠ²Π½ΠΈ осрСднСнной завихрСнности Π½Π°Π±Π»ΡŽΠ΄Π°ΡŽΡ‚ΡΡ Π²Π±Π»ΠΈΠ·ΠΈ ΠΎΠ±Ρ‚Π΅ΠΊΠ°Π΅ΠΌΡ‹Ρ… повСрхностСй ΠΈ Π² ΡƒΠ³Π»ΠΎΠ²Ρ‹Ρ… областях Ρ‚Ρ€Π°Π½ΡˆΠ΅ΠΈ – Ρ‚Π°ΠΌ, Π³Π΄Π΅ происходит ΠΎΡ‚Ρ€Ρ‹Π² ΠΏΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½ΠΎΠ³ΠΎ слоя ΠΈ взаимодСйствиС Π²ΠΈΡ…Ρ€Π΅Π²Ρ‹Ρ… структур слоя смСшСния с ΠΊΠΎΡ€ΠΌΠΎΠ²ΠΎΠΉ стСнкой Ρ‚Ρ€Π°Π½ΡˆΠ΅ΠΈ. ΠœΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ ΠΏΡƒΠ»ΡŒΡΠ°Ρ†ΠΈΠΈ завихрСнности Π½Π°Π±Π»ΡŽΠ΄Π°ΡŽΡ‚ΡΡ Π² области взаимодСйствия Π²ΠΈΡ…Ρ€Π΅Π²Ρ‹Ρ… структур слоя смСшСния с квазиустойчивым ΠΊΡ€ΡƒΠΏΠ½ΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ‹ΠΌ Π²ΠΈΡ…Ρ€Π΅ΠΌ ΠΈ особСнно Π²Π±Π»ΠΈΠ·ΠΈ ΠΊΠΎΡ€ΠΌΠΎΠ²ΠΎΠΉ стСнки

    Pressure fluctuations on the scour surface before prismatic pier

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    The results of experimental research of the wall-pressure fluctuation field acting on the scour surface upstream of the prismatic pier model are presented. Experiments were carried out in the hydraulic flume with an open water surface and sandy bed. The spatial and temporal characteristics of the field of pseudosound the wall-pressure fluctuation were determined on the equilibrium scour surface upstream of the prismatic pier model, as well as the sources of their generation. Two quasistable large-scale horseshoe vortex formations occurred inside the scour hole in front of the bluff body. The first of them were generated in the separation of the boundary layer with the front edge of the scour hole and it formed the upper slope of the scour. A second smaller horseshoe formation were formed by the interaction of the shear layer beyond the scour hole and the down flow along the front surface of the prismatic model and it formed the lower slope of the scour. The highest intensity and level of spectral components of the wall-pressure fluctuation occurred inside the scour hole upstream of the prismatic pier model

    Π’ΠΈΡ…Ρ€ΠΎΠ²Π° Π΄ΠΈΠ½Π°ΠΌΡ–ΠΊΠ° сполучСних Ρ‚Π΅Ρ‡Ρ–ΠΉ

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    Group constructions of bluff bodies are widely used in bridge construction practice. The junction flows of such structures are characterized by considerable complexity, nonstationarity and instability. In the vicinity of bluff bodies, systems of horseshoe vortex structures, shear layers, separated regions, jet flows, wake vortices and vortex Karman’s streets are formed. The study of the features of the generation and evolution of vortex and jet flows, the mechanisms of interaction of these flows with streamlined surfaces requires considerable effort during numerical and physical modeling. The purpose of the work is to determine the features of vortex and jet flow in the region of junction of three-row pile grillage with a rigid flat surface. Experimental studies were carried out in laboratory conditions in a hydrodynamic channel, where the three-row group of cylinders was installed on the hydraulically smooth rigid surface. Visual investigations and measurements of the velocity field were carried out inside and around the three-row grillage. The features of the formation and evolution of vortex and jet flows inside and near the cylindrical group were established. Integral and spectral characteristics of the velocity fluctuation field were obtained. Pages of the article in the issue: 25 - 28 Language of the article: UkrainianΠ“Ρ€ΡƒΠΏΠΎΠ²Ρ– конструкції ΠΏΠΎΠ³Π°Π½ΠΎ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΈΡ… Ρ‚Ρ–Π» ΡˆΠΈΡ€ΠΎΠΊΠΎ Π²ΠΈΠΊΠΎΡ€ΠΈΡΡ‚ΠΎΠ²ΡƒΡŽΡ‚ΡŒΡΡ Ρƒ мостобудівній ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ†Ρ–. Π‘ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ– Ρ‚Π΅Ρ‡Ρ–Ρ— Ρ‚Π°ΠΊΠΈΡ… конструкцій Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·ΡƒΡŽΡ‚ΡŒΡΡ Π·Π½Π°Ρ‡Π½ΠΎΡŽ ΡΠΊΠ»Π°Π΄Π½Ρ–ΡΡ‚ΡŽ, Π½Π΅ΡΡ‚Π°Ρ†Ρ–ΠΎΠ½Π°Ρ€Π½Ρ–ΡΡ‚ΡŽ Ρ‚Π° Π½Π΅ΡΡ‚Ρ–ΠΉΠΊΡ–ΡΡ‚ΡŽ. Π’ ΠΎΠΊΠΎΠ»Ρ– ΠΏΠΎΠ³Π°Π½ΠΎ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΈΡ… Ρ‚Ρ–Π» Ρ„ΠΎΡ€ΠΌΡƒΡŽΡ‚ΡŒΡΡ систСми ΠΏΡ–Π΄ΠΊΠΎΠ²ΠΎΠΏΠΎΠ΄Ρ–Π±Π½ΠΈΡ… Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур, зсувні ΡˆΠ°Ρ€ΠΈ, Π²Ρ–Π΄Ρ€ΠΈΠ²Π½Ρ– області, струмСнСві Ρ‚Π΅Ρ‡Ρ–Ρ—, слідні Π²ΠΈΡ…ΠΎΡ€ΠΈ Ρ‚Π° Π²ΠΈΡ…Ρ€ΠΎΠ²Ρ– Π΄ΠΎΡ€Ρ–ΠΆΠΊΠΈ ΠšΠ°Ρ€ΠΌΠ°Π½Π°. ΠœΠ΅Ρ‚Π° Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ – визначСння особливостСй Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΡ— Ρ‚Π° струмСнСвої Ρ‚Π΅Ρ‡Ρ–Ρ— Π² області сполучСння трирядного пального роствСрку Π· ΠΆΠΎΡ€ΡΡ‚ΠΊΠΎΡŽ пласкою ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Π΅ΡŽ. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ– Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ– дослідТСння Π² Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½ΠΈΡ… ΡƒΠΌΠΎΠ²Π°Ρ… Π·Π° допомогою Π²Ρ–Π·ΡƒΠ°Π»Ρ–Π·Π°Ρ†Ρ–Ρ— Ρ‚Π° Π²ΠΈΠΌΡ–Ρ€ΡŽΠ²Π°Π½Π½Ρ ΠΏΠΎΠ»Ρ–Π² ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– сполучСної Ρ‚Π΅Ρ‡Ρ–Ρ—. Π’ΠΈΠ·Π½Π°Ρ‡Π΅Π½ΠΎ ΠΌΠ΅Ρ…Π°Π½Ρ–Π·ΠΌ Π³Π΅Π½Π΅Ρ€Π°Ρ†Ρ–Ρ— Ρ‚Π° Π΅Π²ΠΎΠ»ΡŽΡ†Ρ–Ρ— Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… Ρ– струмСнСвих Ρ‚Π΅Ρ‡Ρ–ΠΉ. ΠžΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– Ρ–Π½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½Ρ– Ρ‚Π° ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½Ρ– характСристики поля ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– Π² ΠΎΠΊΠΎΠ»Ρ– ΠΏΠ΅Ρ€Π΅Π΄Π½ΡŒΠΎΡ— Π³Ρ€ΡƒΠΏΠΈ Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€Ρ–Π² трирядного роствСрку

    Feature of the vortex and the jet flows around and inside the three-row pile group

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    In this article the results of experimental research of kinematics and the dynamics of horseshoe vortex structures, wake vortices and lateral jet flows, formed around and inside the pile group of three-row grillage, set on a flat rigid surface and sand soil, are presented. Visualization of flow is conducted using water soluble coatings and contrast substances, introduced into the stream. The fields of velocity, pressure and shear stresses around and inside the pile construction were investigated using the miniature sensors of the velocity, dynamic pressure and pressure fluctuations. The place of formation and features of development of large-scale horseshoe vortex structures and wake vortices, and the hydrodynamic characteristics of the vortex and jet flow were determined. The space-time correlation and spectral characteristics of the velocity and pressure fluctuations were measured. The scale of the coherent vortex structures, their frequencies of rotations and oscillations, convective velocities and direction of transfer were determined. The three-dimensional spectrograms and correlograms of vortex and the jet flow about and inside the three-row pile grillage were obtained

    Effect of Fluid Viscosity on Noise of Bileaflet Prosthetic Heart Valve

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    Background. Numerical simulation and experimental research have been used as powerful tools to understand and predict the behavior and mechanics of the operation of natural heart valves and their prostheses in natural and pathoΒ­logical conditions. Such studies help to evaluate the effectiveness of the valves, their design and the results of surgical procedures, to diagnose healthy and impaired function of the heart valves. There is an actual problem in creating more reliable methods and tools for the operation diagnostics of mechanical heart valves. Objective. The aim of the research is to investigate the effect of fluid viscosity on the hydroacoustic characteristics of jets that flow from a semi-closed and open mechanical bileaflet heart valve. To study the possibility of using hydroΒ­acoustic measuring instruments as diagnostic equipment for determining the working conditions of the bileaflet proΒ­stheΒ­tic heart valve. Methods. The experimental research was carried out by means of hydroacoustic measurements of the hydrodynamic noise in the near wake of the side and central jets of the glycerin solution and the pure water flow downstream of the prosthetic bileaflet heart valve. Results. The effect of fluid viscosity on the hydroacoustic characteristics of the jets that flow from a semi-closed and open mechanical bileaflet heart valve has been experimentally determined. Integral and spectral characteristics of the hydrodynamic noise of jets of the glycerin solution and the pure water flow downstream of the bileaflet mitral heart valve for different fluid rate were detected. Conclusions. In the stream conditions of pure water, the integral characteristics of the pressure field are lower than in stream conditions of the aqueous glycerin solution. As the glycerin concentration in the solution increases, increase average pressures and especially RMS pressure fluctuations. The spectral levels of the hydrodynamic noise in the near wake of the side jet of the glycerin solution are lower than for water flow in the frequency ranges from 1 to 7-8 Hz and from 100 to 1000 Hz for fluid rate 5 l/min. For higher fluid rates, the spectral components of the hydrodynamic noise in the near wake of the side jet of the glycerin solution of the semi-closed mitral valve are higher than that for the pure water. The greatest difference (1.5–1.8 times) in the spectral levels is observed in the frequency range from 10 to 100 Hz for the fluid rate 15 l/min

    Π“Ρ–Π΄Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½Ρ– характСристики Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΠ³ΠΎ Ρ€ΡƒΡ…Ρƒ усСрСдині напівсфСричної Π»ΡƒΠ½ΠΊΠΈ

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    Π£ Ρ€ΠΎΠ±ΠΎΡ‚Ρ– прСдставлСні Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΈΡ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ особливостСй формування Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур усСрСдині напівсфСричної Π»ΡƒΠ½ΠΊΠΈ Π½Π° Π³Ρ–Π΄Ρ€Π°Π²Π»Ρ–Ρ‡Π½ΠΎ Π³Π»Π°Π΄ΠΊΡ–ΠΉ плоскій ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ–, поля ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– Ρ‚Π° тиску, які Π²ΠΎΠ½ΠΈ Π³Π΅Π½Π΅Ρ€ΡƒΡŽΡ‚ΡŒ. ЕкспСримСнти проводилися Ρƒ Π³Ρ–Π΄Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½ΠΎΠΌΡƒ Π»ΠΎΡ‚ΠΊΡƒ Π·Π° допомогою Π²Ρ–Π·ΡƒΠ°Π»Ρ–Π·Π°Ρ†Ρ–Ρ— Ρ‚Π΅Ρ‡Ρ–Ρ— Ρ‚Π° Π²ΠΈΠΌΡ–Ρ€ΡŽΠ²Π°Π½Π½Ρ поля ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉ ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ–, Π΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½ΠΎΠ³ΠΎ Ρ– пристінного тиску Π·Π° допомогою Ρ‚Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€Ρ–Π² Ρ‚Π° ΠΌΡ–Π½Ρ–Π°Ρ‚ΡŽΡ€Π½ΠΈΡ… ΠΏ'Ρ”Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΡ–Ρ‡Π½ΠΈΡ… Π΄Π°Ρ‚Ρ‡ΠΈΠΊΡ–Π² тиску. Візуалізація контрастними Π±Π°Ρ€Π²Π½ΠΈΠΊΠ°ΠΌΠΈ Ρ‚Π° Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ·Ρ‡ΠΈΠ½Π½ΠΈΠΌΠΈ покриттями ΠΏΠΎΠΊΠ°Π·Π°Π»Π°, Ρ‰ΠΎ усСрСдині Π»ΡƒΠ½ΠΊΠΈ Π³Π΅Π½Π΅Ρ€ΡƒΡŽΡ‚ΡŒΡΡ квазістійкі Π²Π΅Π»ΠΈΠΊΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ– Π²ΠΈΡ…Ρ€ΠΎΠ²Ρ– структури Ρ– Π΄Ρ€Ρ–Π±Π½ΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ– Π²ΠΈΡ…ΠΎΡ€ΠΈ, які Π²ΠΈΠΊΠΈΠ΄Π°ΡŽΡ‚ΡŒΡΡ Π½Π°Π·ΠΎΠ²Π½Ρ– Π· Π»ΡƒΠ½ΠΊΠΈ. ΠžΡΠΎΠ±Π»ΠΈΠ²ΠΎΡΡ‚Ρ– Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΡ— Ρ‚Π΅Ρ‡Ρ–Ρ— усСрСдині Π»ΡƒΠ½ΠΊΠΈ ΠΎΠ±ΡƒΠΌΠΎΠ²Π»ΡŽΡŽΡ‚ΡŒ появу дискрСтних ΠΏΡ–Π΄ΠΉΠΎΠΌΡ–Π² Ρƒ частотних Ρ‚Π° Ρ…Π²ΠΈΠ»ΡŒΠΎΠ²ΠΈΡ… спСктрах ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– Ρ– тиску Π½Π° частотах Π½ΠΈΠ·ΡŒΠΊΠΎΡ‡Π°ΡΡ‚ΠΎΡ‚Π½ΠΈΡ… коливань Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΡ— Ρ‚Π΅Ρ‡Ρ–Ρ—, Π½Π° частотах обСртання Ρ– Π²ΠΈΠΊΠΈΠ΄Ρƒ Π²Π΅Π»ΠΈΠΊΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΎΡ— Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΡ— структури Ρ‚Π° Π½Π° частотах Π°Π²Ρ‚ΠΎΠΊΠΎΠ»ΠΈΠ²Π°Π½ΡŒ Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур зсувного ΡˆΠ°Ρ€Ρƒ

    Поля ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Π΅ΠΉ Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΡ— Ρ‚Π΅Ρ‡Ρ–Ρ— усСрСдині ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΎΡ— Π½Π°ΠΏΡ–Π²Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΎΡ— ΠΊΠ°Π½Π°Π²ΠΊΠΈ

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    Π— ΠΌΠ΅Ρ‚ΠΎΡŽ Ρ€ΠΎΠ·Π²ΠΈΡ‚ΠΊΡƒ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ–Π²Β  пасивного кСрування ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΈΠΌΠΈ ΡˆΠ°Ρ€Π°ΠΌΠΈ прСдставлСні Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Β Β Β Β Β Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΈΡ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ Π² Π°Π΅Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½Ρ–ΠΉ Ρ‚Ρ€ΡƒΠ±Ρ– Ρ‚Π°ΠΊΠΈΡ… Ρ–Π½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΈΡ… ΠΊΡ–Π½Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π½ΠΈΡ… характСристик Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΎΠ³ΠΎ Ρ€ΡƒΡ…Ρƒ, як усСрСднСні Ρ‚Π° ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉΠ½Ρ– ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– усСрСдині ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΎΠ±Ρ‚Ρ–Ρ‡Π½ΠΎΡ— Π½Π°ΠΏΡ–Π²Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΎΡ— ΠΊΠ°Π½Π°Π²ΠΊΠΈ Ρ‚Π° Π² Ρ—Ρ— Π±Π»ΠΈΠΆΠ½ΡŒΠΎΠΌΡƒ сліді Π½Π° Π³Ρ–Π΄Ρ€Π°Π²Π»Ρ–Ρ‡Π½ΠΎ Π³Π»Π°Π΄ΠΊΡ–ΠΉ пласкій ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ–. НавСдСні Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π²Ρ–Π·ΡƒΠ°Π»Ρ–Π·Π°Ρ†Ρ–Ρ— Ρ‚Π΅Ρ‡Ρ–Ρ— усСрСдині ΠΊΠ°Π½Π°Π²ΠΊΠΈ Ρ– Ρ—Ρ— ΠΎΠΊΠΎΠ»Ρ– для ΠΏΠ΅Ρ€Π΅Ρ…Ρ–Π΄Π½ΠΎΠ³ΠΎ Ρ€Π΅ΠΆΠΈΠΌΡƒ Ρ‚Π΅Ρ‡Ρ–Ρ— Π² ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠΌΡƒ ΡˆΠ°Ρ€Ρ– Π½Π° пластині, ΠΏΠΎΠΊΠ°Π·Π°Π½Ρ– особливості Π³Π΅Π½Π΅Ρ€Π°Ρ†Ρ–Ρ— Π²Π΅Π»ΠΈΠΊΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΈΡ… Π²ΠΈΡ…Ρ€ΠΎΠ²ΠΈΡ… структур усСрСдині ΠΊΠ°Π½Π°Π²ΠΊΠΈ Ρ‚Π° Π²ΠΈΠΊΠΈΠ΄Ρƒ Ρ—Ρ… Π½Π°Π·ΠΎΠ²Π½Ρ– Π· ΠΊΠ°Π½Π°Π²ΠΊΠΈ. Π’Π΅Ρ€ΠΌΠΎΠ°Π½Π΅ΠΌΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π½Ρ– дослідТСння Π΄ΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΈ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Ρ‚ΠΈ поля ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Π΅ΠΉ Ρ‚Π° Ρ„ΡƒΠ½ΠΊΡ†Ρ–Ρ— Ρ‰Ρ–Π»ΡŒΠ½ΠΎΡΡ‚Ρ– Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»Ρƒ ймовірності ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉ ΠΏΠΎΠ·Π΄ΠΎΠ²ΠΆΠ½ΡŒΠΎΡ— ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ–, Ρ—Ρ… ΠΊΠΎΠ΅Ρ„Ρ–Ρ†Ρ–Ρ”Π½Ρ‚ΠΈ асимСтрії Ρ‚Π° СксцСсу Ρƒ сСрСдинному ΠΏΠ΅Ρ€Π΅Ρ€Ρ–Π·Ρ– ΠΊΠ°Π½Π°Π²ΠΊΠΈ. По профілям ΠΏΠΎΠ·Π΄ΠΎΠ²ΠΆΠ½ΡŒΠΎΡ— ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– ΠΏΠΎΠ±ΡƒΠ΄ΠΎΠ²Π°Π½ΠΎ Π»Ρ–Π½Ρ–Ρ— Ρ€Ρ–Π²Π½ΠΈΡ… усСрСднСних Ρ– ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉΠ½ΠΈΡ… складових ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– усСрСдині ΠΊΠ°Π½Π°Π²ΠΊΠΈ. Показано області Π³Π΅Π½Π΅Ρ€Π°Ρ†Ρ–Ρ— Π·Π²ΠΎΡ€ΠΎΡ‚Π½ΠΎΡ— Ρ‚Π΅Ρ‡Ρ–Ρ— усСрСдині ΠΊΠ°Π½Π°Π²ΠΊΠΈ, ΠΏΠΎΠ»Π΅ ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– Ρƒ зсувному ΡˆΠ°Ρ€Ρ– Ρ– області ΠΉΠΎΠ³ΠΎ Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Π· ΠΊΠΎΡ€ΠΌΠΎΠ²ΠΎΡŽ ΡΡ‚Ρ–Π½ΠΊΠΎΡŽ ΠΊΠ°Π½Π°Π²ΠΊΠΈ. ВстановлСно, Ρ‰ΠΎ Π² ΠΏΡ€ΠΈΠΌΠ΅ΠΆΠΎΠ²ΠΎΠΌΡƒ ΡˆΠ°Ρ€Ρ– Π½Π°Π΄ заглиблСнням Π·Π°ΠΊΠΎΠ½ Ρ‰Ρ–Π»ΡŒΠ½ΠΎΡΡ‚Ρ– Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»Ρƒ ймовірності ΠΏΡƒΠ»ΡŒΡΠ°Ρ†Ρ–ΠΉ ΠΏΠΎΠ·Π΄ΠΎΠ²ΠΆΠ½ΡŒΠΎΡ— ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚Ρ– близький Π΄ΠΎ Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ, Π° Π² Π·Π°Π³Π»ΠΈΠ±Π»Π΅Π½Π½Ρ– – Π΄ΠΎ ΠΌΠ°ΠΊΡΠ²Π΅Π»Π»Ρ–Π²ΡΡŒΠΊΠΎΠ³ΠΎ.
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