282 research outputs found
Numerical simulation of heat and mass transfer under the conditions of phase transitions and chemical reaction during ignition of condensed substances by single hot particles
Physical and mathematical models of heat and mass transfer under the conditions of phase transitions and chemical reactions have been developed for the numerical analysis of condensed substances ignition by a single particle (size from 0.5 mm to 5 mm) heated up to high temperature (above 800 K). Liquid, solid and gel fuels were considered as condensed substances. Metal and non-metal particles were used as ignition sources. A heat and mass transfer mathematical model is presented as a system of nonlinear non-stationary differential equations in the private derivatives corresponding to the basic provisions of the general theory of heat transfer in chemical kinetics and free convection. An algorithm for solving differential equations with the corresponding initial and boundary conditions is based on the finite- difference method. The locally one-dimensional method was used to solve difference analogous of differential equations. One-dimensional difference equations were solved using an implicit four-point difference scheme. Nonlinear equations were solved by the iteration method. Mathematical model verification and the assessment of numerical research results reliability was executed by its comparison with experimental results. Also the verification of the law of conservation of energy in the solution area of the ignition problem was performed. Besides, testing of applied numerical methods and the
developed silving algorithm on the example of a group of less complex challenges of thermal conduction and thermal convection was held. The minimum parameters of hot particles (temperature, size) and the ignition delay time of condensed substances were determined for local heat sources with different shapes. The influence of thermal conduction, convection and radiative heat transfer mechanisms in the βparticle β condensed substanceβ system was established on the ignition characteristics
Numerical simulation of water and water emulsion droplets evaporation in flames with different temperatures
The models of heat and mass transfer and phase transition for βwater droplet β flameβ system have been developed using non-stationary nonlinear partial differential equations. The system of differential equations was solved by the finite-difference method. The locally one-dimensional method was used to solve the difference analogous of differential equations. One-dimensional differential equations were solved using an implicit four-point difference scheme. Nonlinear equations were solved by the iteration method. The evaporation rates of water droplets (with sizes from 0.05 mm to 5 mm) in the flame zone (at the temperatures from 500 K to 1200 K) were determined. Theoretical analysis established essentially nonlinear (close to exponential) form of dependence of the water droplet evaporation rate on the temperature of the external gas area and the temperature of a droplet surface. In particular, the water droplet evaporation rate varies from 0.25 to 0.29 kg/(m2s), when the temperature of external gas area is about 1100 K. On the other hand, the water droplet evaporation rate does not exceed 0.01 kg/(m2s) when the temperature of external gas area is about 350 K. Besides, it has been found out that droplets warm up at different rates depending on their initial temperature and velocity. As a result, the integral characteristics of droplet evaporation can increase substantially, when droplets move through the external gas area at the same temperature. We performed a similar investigation or droplet streams with droplet concentration 0.001β0.005 m3 in 1 m3 of gas area (typical parameters for modern spray extinguishing systems)
Individual and synergistic effects of modifications of the carrier medium of carbon-containing slurries on the viscosity and sedimentation stability
The study is devoted to revealing the individual and synergistic effects of modifications of the carrier medium of the coal-water slurries (CWS) based on coking coal and carbon-containing flotation wastes of this coal on the effective viscosity and sedimentation stability. Synthetic and natural wetting agents as well as liquid solvents (alcohol, oil, conventional liquid fuel, methyl ethers) and solid organic compounds exemplified by sawdust are used for this. The relationships between the effective viscosity, water separation ratio, and zeta potential for the CWS with the separate addition of a wetting agent and a solvent is established. The categories of fuel compositions are identified according to the βstabilityβ criterion. The synergistic effect of the additions of a wetting agent and a solvent on the sedimentation stability and effective viscosity is demonstrated. The physicochemical model of interaction between the solid particles and the additives in CWSs is proposed
Remaining life definition of crane metal construction on value of coercive forces
In this work, the condition definition of bridge crane metal construction and prognostication of its remaining life on the basis of nondestructive control method by using coercive forces is presented. Basic approaches and performance stages of the magnetic control for the purpose of metal condition definition and remaining life of its work are considere
Droplet evaporation in water jet at the motion through high temperature gases
Abstract. Heat and mass transfer model for the numerical investigation of the evaporation process of a single droplet in water jet when moving through high temperature gases was developed. The integral characteristics of the process under investigation were calculated. The macroscopic regularities of water droplet evaporation, as elements of jet, in the high temperature gas mixture (as exemplified by combustion products of typical condensed substances) were determined
Numerical Investigation of Water Droplets Shape Influence on Mathematical Modeling Results of Its Evaporation in Motion through a High-Temperature Gas
The numerical investigation of influence of a single water droplet shape on the mathematical modeling results of its evaporation in motion through high-temperature gases (combustion products of a typical condensed substance) has been executed. Values of evaporation time, motion velocity, and distance passed by various droplet shapes (cylinder, sphere, hemisphere, cone, and ellipsoid) in a high-temperature gases medium were analyzed. Conditions have been defined when a droplet surface configuration affects the integrated characteristics of its evaporation, besides temperature and combustion products concentration in a droplet trace, insignificantly. Experimental investigations for the verification of theoretical results have been carried out with using of optical diagnostic methods for two-phase gas-vapor-liquid flows
β2D Planar Simulation of Collisions between Liquid Droplets and βSolid Particles in a Gas
Here we present a 2D planar simulation of the collisions between liquid droplets and solid particles that are most often used in industrial applications. The collisions are modeled using a combination of Volume of Fluid and Level Set methods. We study the impact of the particle-to-droplet size ratio and the shape of solid particles on the collision behavior and interaction regimes. The findings are presented in the form of collision regime maps. The interaction regimes are also distinguished for binary droplet collisions: deposition, separation, and disintegration. We show the impact of density, viscosity, and surface tension on the droplet collision regime maps as well as on the number of secondary fragments. The practical value of the research comes from the newly established differences of collision regimes between droplets and particles of different shapes and sizes
Experimental demonstration of scalable quantum key distribution over a thousand kilometers
Secure communication over long distances is one of the major problems of
modern informatics. Classical transmissions are recognized to be vulnerable to
quantum computer attacks. Remarkably, the same quantum mechanics that engenders
quantum computers offers guaranteed protection against such attacks via quantum
key distribution (QKD). Yet, long-distance transmission is problematic since
the essential signal decay in optical channels occurs at a distance of about a
hundred kilometers. We propose to resolve this problem by a QKD protocol,
further referred to as the Terra Quantum QKD protocol (TQ-QKD protocol). In our
protocol, we use semiclassical pulses containing enough photons for random bit
encoding and exploiting erbium amplifiers to retranslate photon pulses and, at
the same time, ensuring that at the chosen pulse intensity only a few photons
could go outside the channel even at distances of about a hundred meters. As a
result, an eavesdropper will not be able to efficiently utilize the lost part
of the signal. The central component of the TQ-QKD protocol is the end-to-end
loss control of the fiber-optic communication line since optical losses can in
principle be used by the eavesdropper to obtain the transmitted information.
However, our control precision is such that if the degree of the leak is below
the detectable level, then the leaking states are quantum since they contain
only a few photons. Therefore, available to the eavesdropper parts of the bit
encoding states representing `0' and `1' are nearly indistinguishable. Our work
presents the experimental demonstration of the TQ-QKD protocol allowing quantum
key distribution over 1079 kilometers. Further refining the quality of the
scheme's components will expand the attainable transmission distances. This
paves the way for creating a secure global QKD network in the upcoming years.Comment: 23 pages (main text: 15 pages, supplement: 8 pages), 21 figures (main
text: 7 figures, supplement: 14 figures
ΠΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π° ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎ-Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ Π΄Π»Ρ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ ΡΡΠ°Π»Π΅ΠΉ
Contactless electromagnetic-acoustic transducers have a set of significant advantages over contact transducers, but at the same time they have significant disadvantages that require the development of effective magnetizing devices. Compared to magnetizing devices that are using permanent magnets, electric current magnetization devices are easily removed from the object of testing and cleaned from contamination by metal particles. Unfortunately, such transducers have significant dimensions and weight.A transducer containing a magnetic circuit magnetized by an electric current coil and two independent electromagnetic inductors located in the gap between the central part of the magnetic circuit and the object of testing has been developed. Inductors are two flat coils, each of them has form like a butterfly. The inductor conductors located in the working area have mutually perpendicular directions; they allow exciting and receiving the transversely polarized acoustic waves without rearranging the transducer. In order to reduce the overall dimensions and mass of the transducer, the mass and dimensional parameters of the magnetizing device were optimized for operating conditions when the magnetization of the object of testing and measurement are performed during the active measurement phase. During the passive measurement phase, which is three times longer than the active phase in time, the magnetizing device cools down. The cyclic mode with alternating active and passive phases made it possible to reduce the weight of the transducer by more than 3 times. In the working area of the transducer with a size of 15Γ15 mm, with a gap of 1 mm between the magnetic field concentrator and the object of testing, a field with a normal component of 2.4 T is created. The transducer has protection of the magnetization device from overheating, and the cyclic mode of operation allows for continuous performance of up to 30 measurements per minute at an ambient temperature of 20 Β°C.The developed magnetizing device can be used in solving a number of problems of structuroscopy, thickness measurement, flaw detection by electromagnetic-acoustic methods based on accurate measurement of the propagation time of elastic waves in the object of testing.Β ΠΠ΅ΡΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΡΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎ-Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»ΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π½Π°Π±ΠΎΡΠΎΠΌ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ² ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ½ΡΠΌΠΈ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»ΡΠΌΠΈ, Π½ΠΎ ΠΏΡΠΈ ΡΡΠΎΠΌ Ρ Π½ΠΈΡ
Π΅ΡΡΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠ΅ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΊΠΈ, ΡΡΠ΅Π±ΡΡΡΠΈΠ΅ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°ΡΡΠΈΡ
ΡΡΡΡΠΎΠΉΡΡΠ². ΠΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΡΡΡΠΎΠΉΡΡΠ²Π°ΠΌΠΈ Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°Π½ΠΈΡ Π½Π° ΠΏΠΎΡΡΠΎΡΠ½Π½ΡΡ
ΠΌΠ°Π³Π½ΠΈΡΠ°Ρ
ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°Π½ΠΈΡ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΎΠΊΠΎΠΌ Π»Π΅Π³ΠΊΠΎ ΡΠ½ΠΈΠΌΠ°ΡΡΡΡ Ρ ΠΎΠ±ΡΠ΅ΠΊΡΠ° ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΠΈ ΠΎΡΠΈΡΠ°ΡΡΡΡ ΠΎΡ Π·Π°Π³ΡΡΠ·Π½Π΅Π½ΠΈΡ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ°ΡΡΠΈΡΠ°ΠΌΠΈ. Π ΡΠΎΠΆΠ°Π»Π΅Π½ΠΈΡ, ΡΠ°ΠΊΠΈΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»ΠΈ ΠΈΠΌΠ΅ΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ Π³Π°Π±Π°ΡΠΈΡΡ ΠΈ ΠΌΠ°ΡΡΡ.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΠΉ ΠΌΠ°Π³Π½ΠΈΡΠΎΠΏΡΠΎΠ²ΠΎΠ΄, Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°Π΅ΠΌΡΠΉ ΠΊΠ°ΡΡΡΠΊΠΎΠΉ Ρ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΎΠΊΠΎΠΌ, ΠΈ Π΄Π²Π° Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΡ
ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΈΠ½Π΄ΡΠΊΡΠΎΡΠ°, ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½ΡΡ
Π² Π·Π°Π·ΠΎΡΠ΅ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠ΅Π½ΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°ΡΡΡΡ ΠΌΠ°Π³Π½ΠΈΡΠΎΠΏΡΠΎΠ²ΠΎΠ΄Π° ΠΈ ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠΌ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ. ΠΠ½Π΄ΡΠΊΡΠΎΡΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ Π΄Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΠ΅ ΠΊΠ°ΡΡΡΠΊΠΈ, ΠΊΠ°ΠΆΠ΄Π°Ρ ΠΈΠ· ΠΊΠΎΡΠΎΡΡΡ
Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° Π² Π²ΠΈΠ΄Π΅ Π±Π°Π±ΠΎΡΠΊΠΈ. ΠΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΈ ΠΈΠ½Π΄ΡΠΊΡΠΎΡΠΎΠ², ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½ΡΠ΅ Π² ΡΠ°Π±ΠΎΡΠ΅ΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ, ΠΈΠΌΠ΅ΡΡ Π²Π·Π°ΠΈΠΌΠ½ΠΎ ΠΏΠ΅ΡΠΏΠ΅Π½Π΄ΠΈΠΊΡΠ»ΡΡΠ½ΡΠ΅ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ; Ρ ΠΈΡ
ΠΏΠΎΠΌΠΎΡΡΡ ΠΌΠΎΠΆΠ½ΠΎ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π°ΡΡ ΠΈ ΡΠ΅Π³ΠΈΡΡΡΠΈΡΠΎΠ²Π°ΡΡ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΠΎ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΠ΅ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π²ΠΎΠ»Π½Ρ Π±Π΅Π· ΠΏΠ΅ΡΠ΅ΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ. Π‘ ΡΠ΅Π»ΡΡ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ Π³Π°Π±Π°ΡΠΈΡΠ½ΡΡ
ΡΠ°Π·ΠΌΠ΅ΡΠΎΠ² ΠΈ ΠΌΠ°ΡΡΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ ΠΏΡΠΎΠΈΠ·Π²Π΅Π΄Π΅Π½Π° ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΡ ΠΌΠ°ΡΡΠΎΠ³Π°Π±Π°ΡΠΈΡΠ½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π΄Π»Ρ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΡΠΊΡΠΏΠ»ΡΠ°ΡΠ°ΡΠΈΠΈ, ΠΊΠΎΠ³Π΄Π° Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°Π½ΠΈΠ΅ ΠΎΠ±ΡΠ΅ΠΊΡΠ° ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΡΡ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΡΠ°Π·Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ. ΠΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΠ°ΡΡΠΈΠ²Π½ΠΎΠΉ ΡΠ°Π·Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ, Π² ΡΡΠΈ ΡΠ°Π·Π° ΠΏΡΠ΅Π²ΡΡΠ°ΡΡΠ΅ΠΉ Π°ΠΊΡΠΈΠ²Π½ΡΡ ΡΠ°Π·Ρ ΠΏΠΎ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ, ΠΏΡΠΎΠΈΡΡ
ΠΎΠ΄ΠΈΡ ΠΎΡΡΡΠ²Π°Π½ΠΈΠ΅ Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π°. Π¦ΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ΅ΠΆΠΈΠΌ Ρ ΡΠ΅ΡΠ΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΠΈ ΠΏΠ°ΡΡΠΈΠ²Π½ΠΎΠΉ ΡΠ°Π· ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΠΌΠ΅Π½ΡΡΠΈΡΡ Π²Π΅Ρ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ Π±ΠΎΠ»Π΅Π΅ ΡΠ΅ΠΌ Π² 3 ΡΠ°Π·Π°. Π ΡΠ°Π±ΠΎΡΠ΅ΠΉ Π·ΠΎΠ½Π΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠΌ 15Γ15 ΠΌΠΌ ΠΏΡΠΈ Π·Π°Π·ΠΎΡΠ΅ Π² 1 ΠΌΠΌ ΠΌΠ΅ΠΆΠ΄Ρ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΎΡΠΎΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ ΠΈ ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠΌ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΡΠΎΠ·Π΄Π°ΡΡΡΡ ΠΏΠΎΠ»Π΅ Ρ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠΎΠΉ Π² 2,4 Π’Π».ΠΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ ΡΠΎΠ΄Π΅ΡΠΆΠΈΡ Π·Π°ΡΠΈΡΡ ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°Π½ΠΈΡ ΠΎΡ ΠΏΠ΅ΡΠ΅Π³ΡΠ΅Π²Π°, Π° ΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ΅ΠΆΠΈΠΌ ΡΠ°Π±ΠΎΡΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΡΡ Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΡΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ Π΄ΠΎ 30 ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π² ΠΌΠΈΠ½ΡΡΡ ΠΏΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅ ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ ΡΡΠ΅Π΄Ρ 20 ΒΊΠ‘.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠ΅ Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠΈΠ²Π°ΡΡΠ΅Π΅ ΡΡΡΡΠΎΠΉΡΡΠ²ΠΎ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΎ ΠΏΡΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ ΡΡΠ΄Π° Π·Π°Π΄Π°Ρ ΡΡΡΡΠΊΡΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΌΠ΅ΡΡΠΈΠΈ, Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎ-Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠΌΠΈ Π½Π° ΡΠΎΡΠ½ΠΎΠΌ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΈ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΡ ΡΠΏΡΡΠ³ΠΈΡ
Π²ΠΎΠ»Π½ Π² ΠΎΠ±ΡΠ΅ΠΊΡΠ΅ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ
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