Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824603772
Yu. D. Chashechkin, A. Yu. Il’inykh
{"title":"Submerging and Floating-up Vortices in the Picture of Smooth Inflow of a Free-Falling Ethanol Drop into Water","authors":"Yu. D. Chashechkin, A. Yu. Il’inykh","doi":"10.1134/S0015462824603772","DOIUrl":"10.1134/S0015462824603772","url":null,"abstract":"<p>The comparative videorecording of the coalescence pictures of free falling drops of 0.01% water solution of potassium permanganate and 95% ethanol solution of smaller density is performed. The kinetic energy of both fluids is smaller than the potential surface energy. The drop of the solution, whose density is greater than that of the target fluid, flows smoothly into the fluid thickness, while a cavity is formed with retardation. The submerging intrusion transforms into an annular vortex, which is pushed by a growing cavity. The ethanol drop also flows into the fluid thickness but forms a floating-up intrusion, which distorts the shape of the target cavity. When the conical cavity stops to sharpen and attains a maximum depth, a small vortex, which contains the light fluid, is thrown into the fluid thickness. The dimensions of the vortex forming the secondary intrusion remain almost the same during the motion. The light vortex stops gradually and forms the secondary intrusion. The central region of the secondary intrusion floats up and transforms into a vortex ring. The dimensions of the buoyancy-driven floating-up vortex increase with time. The time dependences of the dimensions of the basic structural components are presented.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1789 - 1808"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423072","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824604613
D. V. Antonov, R. M. Fedorenko, D. N. Kovalev, P. A. Strizhak
{"title":"Energy Balance of Puffing and Microexplosion of Two-Liquid Droplets","authors":"D. V. Antonov, R. M. Fedorenko, D. N. Kovalev, P. A. Strizhak","doi":"10.1134/S0015462824604613","DOIUrl":"10.1134/S0015462824604613","url":null,"abstract":"<p>The results of energy analysis of the fragmentation regimes (puffing and microexplosion) of two-liquid droplets of the core-shell type are given. It is shown that using the classical energy approach to describe the hydrodynamic processes, it is possible to predict the critical (necessary and sufficient) conditions for the implementation of fragmentation regimes and their consequences. As distinct from the force approach, it is possible to estimate the discrete energies spent on evaporation, heating, fragmentation, viscous dissipation, and resistance during the motion of the fragmentation front.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1751 - 1764"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423143","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824604297
V. V. Zaviyalov
{"title":"An Exact Solution for a Time-Dependent System of Radiative-Conductive Heat Transfer Equations","authors":"V. V. Zaviyalov","doi":"10.1134/S0015462824604297","DOIUrl":"10.1134/S0015462824604297","url":null,"abstract":"<p>An exact self-similar solution of the type of a traveling heat wave for the time-dependent nonlinear system of radiative-conductive heat transport equations in the Cartesian geometry is considered. The radiation component is considered in the kinetic model with specially adjusted absorption and scattering coefficients. An example of the test problem in the plane geometry is given.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1735 - 1740"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423069","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824603747
A. V. Palagin
{"title":"Exact Solution of the Problem of Vapor Flow in a Gap between an Evaporating Droplet of Liquid and a Hot Wall","authors":"A. V. Palagin","doi":"10.1134/S0015462824603747","DOIUrl":"10.1134/S0015462824603747","url":null,"abstract":"<p>Vapor flow in a gap between a liquid droplet and a hot wall caused by evaporation of liquid is considered. It is assumed that the wall temperature is higher than the minimum film boiling temperature, and there is no direct contact with liquid. In particular, the problem of such a flow arises in modeling post-dryout heat transfer, when droplets from a vapor–liquid flow fall onto the heated surface and partially evaporate on it, making a significant contribution to heat transfer. Within the framework of the problem under consideration, the gap between the droplet and the wall is assumed to be plane, and the vapor flow to be laminar and axisymmetric. An exact solution to the corresponding hydrodynamic problem is given.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1779 - 1788"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423071","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824603735
I. K. Gimaltdinov, A. S. Rodionov, O. Yu. Valiakhmetova
{"title":"Evolution of Pressure Waves in Liquid Containing a Porous Partition Saturated with a Bubble Fluid","authors":"I. K. Gimaltdinov, A. S. Rodionov, O. Yu. Valiakhmetova","doi":"10.1134/S0015462824603735","DOIUrl":"10.1134/S0015462824603735","url":null,"abstract":"<p>The distinctive features of pressure wave dynamics in the presence of a porous partition (layer) saturated with a bubbly fluid are considered. It is shown that, depending on the parameters of the gas mixture and the porous medium (volume gas content, bubble dispersion, and porosity), reflection of a wave pulse from the porous partition saturated with a bubbly mixture is similar to reflection from the free boundary or from the rigid wall.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1869 - 1877"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1134/S0015462824603735.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143422988","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824604315
Yu. D. Chashechkin
{"title":"The Laws of the Matter Distribution in a Colored Free-Falling Drop in a Transparent Target Fluid (Review)","authors":"Yu. D. Chashechkin","doi":"10.1134/S0015462824604315","DOIUrl":"10.1134/S0015462824604315","url":null,"abstract":"<p>The results of the visualization of the matter transfer processes in colored free-fall drops, which mix with a transparent target fluid are analyzed. The parametrization is carried out basing on the system of fundamental equations of fluid mechanics which includes the equations of state for the density and the Gibbs potential. The contribution of different mechanisms of energy transfer is discussed; these are the macroscopic (including flows, waves, and vortices) and microscopic (dissipative and conversional) ones. The radiation transfer effect is not considered. The technique of the present-day experiments is descried, which allows to record accompanying acoustic signals together with the highly-resolving videorecording of colored flow pictures. The flow structure, dynamics, and energetics are analyzed for different density ratios of the confluent fluids and the kinetic and potential surface energies (PSE) of the drop. The conditions of the establishment of certain selected regimes, such as intrusive drop inflow, impact breakdown in fibers, and an intermediate hovering and rebound regime, are determined. A drop flowing smoothly into the fluid thickness at a small contact velocity in the intrusive regime forms a connected body. Thin trickles containing the matter of both media are formed in the contact spot in the impact mode. The fibrous wakes of the trickles form lineate and reticular structures on the fluid surface and within its thickness. In the intermediate regime the drop can hover on the fluid surface, touch it, merge partially with it, and rebound with the loss of the matter. The evolution of gas cavities and bubbles radiating acoustic packets is traced. The necessity of taking account for all the mechanisms of total energy transfer in describing hydrodynamics and acoustics of drop flows is noted.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1693 - 1734"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423070","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824605278
D. V. Georgievskii
{"title":"Sufficient Energy Estimates of Stability of Unsteady Combined Shear Flows in a Cylindrical Layer","authors":"D. V. Georgievskii","doi":"10.1134/S0015462824605278","DOIUrl":"10.1134/S0015462824605278","url":null,"abstract":"<div><p>The time evolution of the three-dimensional pattern of initial disturbances imposed on an unsteady flow, which is a combination of one-dimensional <span>(rtheta )</span>- and <span>(rz)</span>-shears of Newtonian viscous fluid in a cylindrical layer infinite in length, is studied. The annular and axial velocities of both cylindrical boundaries, which do not vary in the disturbed motion, are specified. The formulation of the linearized problem in terms of variations in the velocities, the strain rates, the pressure, and the stress deviator is given. To analyze this problem, the method of integral relations is developed. The method makes it possible to obtain sufficient estimates of the development of disturbances in the Hilbert space H<sub>2</sub>, in particular, Lyapunov stability and asymptotic stability. These estimates include both the kinematic parameters of main flow and harmonics of the annular disturbances and wavenumbers of axial disturbances. For the steady-state main flow in the layer, exponential estimates of stability take place.</p></div>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1765 - 1772"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423077","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824603553
A. O. Gusev, I. A. Denisov, O. S. Mazhorova
{"title":"Numerical Study of Interplay between Double-diffusive Convection and Interfacial Phenomena in Vertical Bridgman Crystal Growth of CdZnTe","authors":"A. O. Gusev, I. A. Denisov, O. S. Mazhorova","doi":"10.1134/S0015462824603553","DOIUrl":"10.1134/S0015462824603553","url":null,"abstract":"<p>The influence of transient heat and mass transfer processes in the melt, crystal and crucible on melt–solid interface shape and solute segregation in Bridgman growth of CdZnTe is investigated numerically. The computations elucidate a crucial role that the radial temperature gradient, formed by an interaction of latent heat release and external heat flux near the interface, plays in the evolution of the interface shape. Analysis of melt motion shows that solutal buoyancy force reduces the intensity of thermally induced convection up to a very low level. As a result, solute distribution in the melt is characteristic of diffusive transport regime. At the advanced stages of the process, when the growth interface moves slowly, and concentration of ZnTe in the melt becomes nearly homogeneous, complete mixing model is suitable for the description of axial ZnTe distribution in the crystal.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1888 - 1904"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423082","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S0015462824604601
A. O. Kokovin, V. Yu. Kozhevnikov, A. V. Kozyrev, N. S. Semenyuk
{"title":"Electrodynamic Mechanism of Expansion of Two-Component Plasma in a Spherically Symmetric Vacuum Gap","authors":"A. O. Kokovin, V. Yu. Kozhevnikov, A. V. Kozyrev, N. S. Semenyuk","doi":"10.1134/S0015462824604601","DOIUrl":"10.1134/S0015462824604601","url":null,"abstract":"<p>The results of theoretical modeling of spherically symmetric expansion of collisionless carbon plasma from a compact explosive emission center of a vacuum discharge are presented. The modeling is based on the joint solution of the Vlasov kinetic equations for electrons and ions and the Poisson equation for the electric field, written in the spherical coordinate system and averaged over angular variables. It is shown that the calculated cathode plasma expansion velocities are significantly lower in the spherically symmetric geometry than the expansion velocities of plasma with the same parameters obtained by solving the plane problem. The observed expansion velocities of the cathode plume plasma at the level of 3.5 × 10<sup>6</sup> cm/s can be explained within the framework of the collisionless mechanism when the criterion imposed on the ratio of the electric emission current to the limiting electric current in the vacuum gap is fulfilled.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1860 - 1868"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423076","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Fluid DynamicsPub Date : 2025-01-10DOI: 10.1134/S001546282460367X
D. V. Knyazev
{"title":"Axisymmetric Poiseuille Flow with Temperature-Dependent Viscosity under Pressure and Temperature Gradients","authors":"D. V. Knyazev","doi":"10.1134/S001546282460367X","DOIUrl":"10.1134/S001546282460367X","url":null,"abstract":"<p>The study of steady-state axisymmetric Poiseuille flow of a Newtonian fluid induced by streamwise pressure and temperature gradients in the case of the dynamic viscosity coefficient dependent on the temperature is reduced to finding solutions to a three-parameter boundary-value problem for a third-order ordinary differential equation. In the domain of the parameter space corresponding to negative axial temperature gradients, there exist two branches of solutions describing flows accompanied by heat removal from the fluid. When the branches meet, they form a boundary in the phase space beyond which no solutions to the Poiseuille-type problem exist. One of the branches can be continued into the domain of non-negative values of the streamwise temperature gradient and contains an isothermal Poiseuille solution. Along this branch, curve of the flow rate as a function of the dimensionless axial temperature gradient has a minimum in the domain of positive values of the latter. In this part of the parameter space, the heat exchange regime with the external medium depends on the relation between all three dimensionless numbers of the problem. The heat exchange regime affects the nature of flow, slowing down the flow near the rigid wall during heat transfer, and forming a more filled velocity profile when heat is absorbed by fluid.</p>","PeriodicalId":560,"journal":{"name":"Fluid Dynamics","volume":"59 6","pages":"1741 - 1750"},"PeriodicalIF":1.0,"publicationDate":"2025-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1134/S001546282460367X.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143423204","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}