27 research outputs found
VARIANT ANATOMY OF INTERCOSTAL NERVES AT THE UMBILICAL REGION IN PERSONS WITH VARIOUS FORMS OF ANTERIOR ABDOMINAL WALL
Objective: the examine variants of quantity of intercostal nerves in the area of the lateral edge rectus sheath around umbilical region, depending on the shape of the anterior abdominal wall. Materials and methods: There were studied 88 floating corpses of both sexes without pathology of the anterior abdominal wall. Among them there were 45% male corpses (mean age β 53,8Β±11,9 years) and 55% β female corpses (51,9Β±13,2 years). We measured linea bicostalis, linea bispinalis and linea xiphoidopubica, determined quantity of the intercostal nerves in the umbilical region of the anterior abdominal wall. Results: At the study of anthropometric parameters of the anterior abdominal wall were found that linea bicostalis averaged 29,2Β±0,3 cm, linea bispinalis β 28,2Β±0,2 cm, linea xiphoidopubica β 30,4Β±0,5 cm. Using method of cluster analysis of the new data were obtained the main shapes of anterior abdominal wall: male, oval, female. It was found that persons with a female shape of the anterior abdominal wall was observed significantly more often 2 pairs of intercostal nerves (74%). In turn, at persons with oval shape were often observed 3 pairs of intercostal nerves (60%). In the cases of the male shape of the anterior abdominal wall 1 pair of intercostal nerves were observed in 38%, and 2 pairs of nerves β in 50% of cases. Conclusions: The quantity of intercostal nerves in the area of the lateral edge rectus sheath around umbilical region depends on the shape of the anterior abdominal wall
Numerical investigation of heat and mass transfer processes in a spherical layer of viscous incompressible liquid with free boundaries
The results of mathematical modelling of the dynamics of a mixture of the viscous incompressible liquid and gas, which fills a spherical layer with free boundaries and contains a gas bubble within itself, are presented in this paper. Spherical symmetry is assumed, and it is considered that the dynamics of the layer is determined by thermal, diffusive and inertial factors. On the basis of constructed numerical algorithm the studies of the formation of the liquid glass layers, which contain the carbon dioxide gas within themselves, have been conducted. The impact of the external thermal regime, external pressure and the density of gas in the bubble at the initial time on the dynamics of the layer, diffusion and heat-and-mass processes inside it is investigated. The results of numerical investigation of the full and simplified thermal problem statement, without consideration of gas diffusion, are compared
The Influence of Gas Diffusion on the Dynamics of A Spherical Layer of Viscous Incompressible Liquid and Heat and Mass Transfer in it
The formation of spherical microballoons in the case of short-term weightlessness is investigated numerically. The algorithm of the numerical solution of the problem is described and the results of numerical studies of the formation of liquid glass microballoons, saturated with carbon dioxide, are presented. The results of calculations for the problem in the full statement (mathematical model includes the influence of inertial, thermal and diffusive factors) and simplified statement, when the process of gas diffusion is not taken into account, are compared
The Influence of Gas Diffusion on the Dynamics of A Spherical Layer of Viscous Incompressible Liquid and Heat and Mass Transfer in it
The formation of spherical microballoons in the case of short-term weightlessness is investigated numerically. The algorithm of the numerical solution of the problem is described and the results of numerical studies of the formation of liquid glass microballoons, saturated with carbon dioxide, are presented. The results of calculations for the problem in the full statement (mathematical model includes the influence of inertial, thermal and diffusive factors) and simplified statement, when the process of gas diffusion is not taken into account, are compared
Investigation of behavior of the dynamic contact angle on the basis of the Oberbeck-Boussinesq approximation of the Navier-Stokes equations
Flows of a viscous incompressible liquid with a thermocapillary boundary are investigated numerically on the basis of the mathematical model that consists of the Oberbeck-Boussinesq approximation of the Navier-Stokes equations, kinematic and dynamic conditions at the free boundary and of the slip boundary conditions at solid walls. We assume that the constant temperature is kept on the solid walls. On the thermocapillary gas-liquid interface the condition of the third order for temperature is imposed. The numerical algorithm based on a finite-difference scheme of the second order approximation on space and time has been constructed. The numerical experiments are performed for water under conditions of normal and low gravity for different friction coefficients and different values of the interphase heat transfer coefficient
Investigation of behavior of the dynamic contact angle on the basis of the Oberbeck-Boussinesq approximation of the Navier-Stokes equations
Flows of a viscous incompressible liquid with a thermocapillary boundary are investigated numerically on the basis of the mathematical model that consists of the Oberbeck-Boussinesq approximation of the Navier-Stokes equations, kinematic and dynamic conditions at the free boundary and of the slip boundary conditions at solid walls. We assume that the constant temperature is kept on the solid walls. On the thermocapillary gas-liquid interface the condition of the third order for temperature is imposed. The numerical algorithm based on a finite-difference scheme of the second order approximation on space and time has been constructed. The numerical experiments are performed for water under conditions of normal and low gravity for different friction coefficients and different values of the interphase heat transfer coefficient
Detecting architectural integrity violation patterns using machine learning
Recent1 years have seen a surge of research into new ways of analyzing software quality. Specifically, a set of studies has been devoted to the impact the architectural relations among files have on system maintainability and file bug-proneness. The literature has proposed a set of rules for deter
Π§ΠΈΡΠ»Π΅Π½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ ΡΠ³Π»Π° ΠΎΡ ΡΠΊΠΎΡΠΎΡΡΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ° Π² Π·Π°Π΄Π°ΡΠ΅ ΠΎ ΠΊΠΎΠ½Π²Π΅ΠΊΡΠΈΠ²Π½ΠΎΠΌ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ
A two-dimensional problem of the fluid flows with a dynamic contact angle is studied in the case of an
uniformly moving contact point. Mathematical modeling of the flows is carried out with the help of the
Oberbeck-Boussinesq approximation of the Navier-Stokes equations. On the thermocapillary free boundary
the kinematic, dynamic conditions and the heat exchange condition of third order are fulfilled. The slip
conditions (conditions of proportionality of the tangential stresses to the difference of the tangential
velocities of liquid and wall) are prescribed on the solid boundaries of the channel supporting by constant
temperature. The dependence of the dynamic contact angle on the contact point velocity is investigated
numerically. The results demonstrate the contact angle behavior and the different flow characteristics
with respect to the various values of the contact point velocity, friction coefficients, gravity acceleration
and an intensity of the thermal boundary regimesΠΠ·ΡΡΠ°Π΅ΡΡΡ Π·Π°Π΄Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ Ρ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΡΠΌ ΡΠ³Π»ΠΎΠΌ Π² ΡΠ»ΡΡΠ°Π΅ ΡΠ°Π²Π½ΠΎΠΌΠ΅ΡΠ½ΠΎ
Π΄Π²ΠΈΠΆΡΡΠ΅ΠΉΡΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°. ΠΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΡΡΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π°ΠΏΠΏΡΠΎΠΊ-
ΡΠΈΠΌΠ°ΡΠΈΠΈ ΠΠ±Π΅ΡΠ±Π΅ΠΊΠ°-ΠΡΡΡΠΈΠ½Π΅ΡΠΊΠ° ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΠ°Π²ΡΠ΅-Π‘ΡΠΎΠΊΡΠ°. ΠΠ° ΡΠ΅ΡΠΌΠΎΠΊΠ°ΠΏΠΈΠ»Π»ΡΡΠ½ΠΎΠΉ ΡΠ²ΠΎΠ±ΠΎΠ΄Π½ΠΎΠΉ Π³ΡΠ°Π½ΠΈ-
ΡΠ΅ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ ΠΊΠΈΠ½Π΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅, Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΈ ΡΡΠ»ΠΎΠ²ΠΈΠ΅ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±ΠΌΠ΅Π½Π° Ρ Π²Π½Π΅ΡΠ½Π΅ΠΉ
ΡΡΠ΅Π΄ΠΎΠΉ ΡΡΠ΅ΡΡΠ΅Π³ΠΎ ΡΠΎΠ΄Π°. Π£ΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠΈΠ»ΠΈΠΏΠ°Π½ΠΈΡ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ Π½Π° ΡΠ²Π΅ΡΠ΄ΡΡ
Π³ΡΠ°Π½ΠΈΡΠ°Ρ
, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΠΎΠ΄Π΄Π΅Ρ-
ΠΆΠΈΠ²Π°ΡΡΡΡ ΠΏΡΠΈ ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅. ΠΠ°Π½Π½ΡΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠΎΠΏΠΎΡ-
ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΠΈ ΠΊΠ°ΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ ΡΠ°Π·Π½ΠΈΡΠ΅ ΠΊΠ°ΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΊΠΎΡΠΎΡΡΠ΅ΠΉ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ ΠΈ ΡΠ²Π΅ΡΠ΄ΠΎΠΉ
ΡΡΠ΅Π½ΠΊΠΈ. Π§ΠΈΡΠ»Π΅Π½Π½ΠΎ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ ΡΠ³Π»Π° ΠΎΡ ΡΠΊΠΎΡΠΎΡΡΠΈ Π΄Π²ΠΈ-
ΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ
ΡΠ³Π»Π° ΠΈ ΡΠ°Π·Π»ΠΈΡΠΈΡ Π² Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°Ρ
ΡΠ΅ΡΠ΅Π½ΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠΊΠΎΡΠΎΡΡΠΈ
Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°, ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΡΠ΅Π½ΠΈΡ, ΡΡΠΊΠΎΡΠ΅Π½ΠΈΡ ΡΠΈΠ»Ρ ΡΡΠΆΠ΅ΡΡΠΈ ΠΈ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎ-
ΡΡΠΈ Π³ΡΠ°Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌ
Π§ΠΈΡΠ»Π΅Π½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ ΡΠ³Π»Π° ΠΎΡ ΡΠΊΠΎΡΠΎΡΡΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ° Π² Π·Π°Π΄Π°ΡΠ΅ ΠΎ ΠΊΠΎΠ½Π²Π΅ΠΊΡΠΈΠ²Π½ΠΎΠΌ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ
A two-dimensional problem of the fluid flows with a dynamic contact angle is studied in the case of an
uniformly moving contact point. Mathematical modeling of the flows is carried out with the help of the
Oberbeck-Boussinesq approximation of the Navier-Stokes equations. On the thermocapillary free boundary
the kinematic, dynamic conditions and the heat exchange condition of third order are fulfilled. The slip
conditions (conditions of proportionality of the tangential stresses to the difference of the tangential
velocities of liquid and wall) are prescribed on the solid boundaries of the channel supporting by constant
temperature. The dependence of the dynamic contact angle on the contact point velocity is investigated
numerically. The results demonstrate the contact angle behavior and the different flow characteristics
with respect to the various values of the contact point velocity, friction coefficients, gravity acceleration
and an intensity of the thermal boundary regimesΠΠ·ΡΡΠ°Π΅ΡΡΡ Π·Π°Π΄Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ Ρ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΡΠΌ ΡΠ³Π»ΠΎΠΌ Π² ΡΠ»ΡΡΠ°Π΅ ΡΠ°Π²Π½ΠΎΠΌΠ΅ΡΠ½ΠΎ
Π΄Π²ΠΈΠΆΡΡΠ΅ΠΉΡΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°. ΠΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΡΡΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π°ΠΏΠΏΡΠΎΠΊ-
ΡΠΈΠΌΠ°ΡΠΈΠΈ ΠΠ±Π΅ΡΠ±Π΅ΠΊΠ°-ΠΡΡΡΠΈΠ½Π΅ΡΠΊΠ° ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΠ°Π²ΡΠ΅-Π‘ΡΠΎΠΊΡΠ°. ΠΠ° ΡΠ΅ΡΠΌΠΎΠΊΠ°ΠΏΠΈΠ»Π»ΡΡΠ½ΠΎΠΉ ΡΠ²ΠΎΠ±ΠΎΠ΄Π½ΠΎΠΉ Π³ΡΠ°Π½ΠΈ-
ΡΠ΅ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ ΠΊΠΈΠ½Π΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅, Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΈ ΡΡΠ»ΠΎΠ²ΠΈΠ΅ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±ΠΌΠ΅Π½Π° Ρ Π²Π½Π΅ΡΠ½Π΅ΠΉ
ΡΡΠ΅Π΄ΠΎΠΉ ΡΡΠ΅ΡΡΠ΅Π³ΠΎ ΡΠΎΠ΄Π°. Π£ΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠΈΠ»ΠΈΠΏΠ°Π½ΠΈΡ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ Π½Π° ΡΠ²Π΅ΡΠ΄ΡΡ
Π³ΡΠ°Π½ΠΈΡΠ°Ρ
, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΠΎΠ΄Π΄Π΅Ρ-
ΠΆΠΈΠ²Π°ΡΡΡΡ ΠΏΡΠΈ ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅. ΠΠ°Π½Π½ΡΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠΎΠΏΠΎΡ-
ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΠΈ ΠΊΠ°ΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ ΡΠ°Π·Π½ΠΈΡΠ΅ ΠΊΠ°ΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΊΠΎΡΠΎΡΡΠ΅ΠΉ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ ΠΈ ΡΠ²Π΅ΡΠ΄ΠΎΠΉ
ΡΡΠ΅Π½ΠΊΠΈ. Π§ΠΈΡΠ»Π΅Π½Π½ΠΎ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ ΡΠ³Π»Π° ΠΎΡ ΡΠΊΠΎΡΠΎΡΡΠΈ Π΄Π²ΠΈ-
ΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΠΎΠ³ΠΎ
ΡΠ³Π»Π° ΠΈ ΡΠ°Π·Π»ΠΈΡΠΈΡ Π² Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°Ρ
ΡΠ΅ΡΠ΅Π½ΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠΊΠΎΡΠΎΡΡΠΈ
Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΡΠΊΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ°, ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΡΠ΅Π½ΠΈΡ, ΡΡΠΊΠΎΡΠ΅Π½ΠΈΡ ΡΠΈΠ»Ρ ΡΡΠΆΠ΅ΡΡΠΈ ΠΈ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎ-
ΡΡΠΈ Π³ΡΠ°Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌ