31 research outputs found
Improved Modeling of Peptide-Protein Binding Through Global Docking and Accelerated Molecular Dynamics Simulations
This work is licensed under a Creative Commons Attribution 4.0 International License.Peptides mediate up to 40% of known protein-protein interactions in higher eukaryotes and play a key role in cellular signaling, protein trafficking, immunology, and oncology. However, it is challenging to predict peptide-protein binding with conventional computational modeling approaches, due to slow dynamics and high peptide flexibility. Here, we present a prototype of the approach which combines global peptide docking using ClusPro PeptiDock and all-atom enhanced simulations using Gaussian accelerated molecular dynamics (GaMD). For three distinct model peptides, the lowest backbone root-mean-square deviations (RMSDs) of their bound conformations relative to X-ray structures obtained from PeptiDock were 3.3β4.8 Γ
, being medium quality predictions according to the Critical Assessment of PRediction of Interactions (CAPRI) criteria. GaMD simulations refined the peptide-protein complex structures with significantly reduced peptide backbone RMSDs of 0.6β2.7 Γ
, yielding two high quality (sub-angstrom) and one medium quality models. Furthermore, the GaMD simulations identified important low-energy conformational states and revealed the mechanism of peptide binding to the target proteins. Therefore, PeptiDock+GaMD is a promising approach for exploring peptide-protein interactions
Study of the impacts of droplets deposited from the gas core onto a gas-sheared liquid film
The results of an experimental study on droplet impactions in the flow of a gas-sheared liquid film are presented. In contrast to most similar studies, the impacting droplets were entrained from film surface by the gas stream. The measurements provide film thickness data, resolved in both longitudinal and transverse coordinates and in time together with the images of droplets above the interface and images of gas bubbles entrapped by liquid film. The parameters of impacting droplets were measured together with the local liquid film thickness. Two main scenarios of droplet-film interaction, based on type of film perturbation, are identified; the parameter identifying which scenario occurs is identified as the angle of impingement. At large angles an asymmetric crater appears on film surface; at shallow angles a long, narrow furrow appears. The most significant difference between the two scenarios is related to possible impact outcome: craters may lead to creation secondary droplets, whereas furrows are accompanied by entrapment of gas bubbles into the liquid film. In addition, occurrence of partial survival of impacting droplet is reported
Prediction of protein assemblies, the next frontier: The CASP14-CAPRI experiment
We present the results for CAPRI Round 50, the fourth joint CASP-CAPRI protein assembly prediction challenge. The Round comprised a total of twelve targets, including six dimers, three trimers, and three higher-order oligomers. Four of these were easy targets, for which good structural templates were available either for the full assembly, or for the main interfaces (of the higher-order oligomers). Eight were difficult targets for which only distantly related templates were found for the individual subunits. Twenty-five CAPRI groups including eight automatic servers submitted ~1250 models per target. Twenty groups including six servers participated in the CAPRI scoring challenge submitted ~190 models per target. The accuracy of the predicted models was evaluated using the classical CAPRI criteria. The prediction performance was measured by a weighted scoring scheme that takes into account the number of models of acceptable quality or higher submitted by each group as part of their five top-ranking models. Compared to the previous CASP-CAPRI challenge, top performing groups submitted such models for a larger fraction (70β75%) of the targets in this Round, but fewer of these models were of high accuracy. Scorer groups achieved stronger performance with more groups submitting correct models for 70β80% of the targets or achieving high accuracy predictions. Servers performed less well in general, except for the MDOCKPP and LZERD servers, who performed on par with human groups. In addition to these results, major advances in methodology are discussed, providing an informative overview of where the prediction of protein assemblies currently stands.Cancer Research UK, Grant/Award Number: FC001003; Changzhou Science and Technology Bureau, Grant/Award Number: CE20200503; Department of Energy and Climate Change, Grant/Award Numbers: DE-AR001213, DE-SC0020400, DE-SC0021303; H2020 European Institute of Innovation and Technology, Grant/Award Numbers: 675728, 777536, 823830; Institut national de recherche en informatique et en automatique (INRIA), Grant/Award Number: Cordi-S; Lietuvos Mokslo Taryba, Grant/Award Numbers: S-MIP-17-60, S-MIP-21-35; Medical Research Council, Grant/Award Number: FC001003; Japan Society for the Promotion of Science KAKENHI, Grant/Award Number: JP19J00950; Ministerio de Ciencia e InnovaciΓ³n, Grant/Award Number: PID2019-110167RB-I00; Narodowe Centrum Nauki, Grant/Award Numbers: UMO-2017/25/B/ST4/01026, UMO-2017/26/M/ST4/00044, UMO-2017/27/B/ST4/00926; National Institute of General Medical Sciences, Grant/Award Numbers: R21GM127952, R35GM118078, RM1135136, T32GM132024; National Institutes of Health, Grant/Award Numbers: R01GM074255, R01GM078221, R01GM093123, R01GM109980, R01GM133840, R01GN123055, R01HL142301, R35GM124952, R35GM136409; National Natural Science Foundation of China, Grant/Award Number: 81603152; National Science Foundation, Grant/Award Numbers: AF1645512, CCF1943008, CMMI1825941, DBI1759277, DBI1759934, DBI1917263, DBI20036350, IIS1763246, MCB1925643; NWO, Grant/Award Number: TOP-PUNT 718.015.001; Wellcome Trust, Grant/Award Number: FC00100
Π¦ΠΠΠΠΠΠ ΠΠΠΠ« ΠΠΠΠ£Π‘ΠΠ Π₯ΠΠΠΠΠΠ‘ΠΠΠΠ ΠΠΠΠΠΠ’ΠΠΠ― ST-25
The results of the start sequence diagram selection and experimental tests of the ST-25 Hall thruster intended for using on small spacecraft are presented. In order to reduce the mass and dimensions of the power processing unit of the propulsion system, it is proposed to exclude the hollow cathode keeper power supply from the structure of the power processing unit. The exclusion of the keeper power supply from the power processing unit made it necessary to select the thruster start sequence diagram. Four start sequence diagrams of the ST-25 Hall thruster start-up are considered: a) using a separate high voltage power supply for the hollow cathode keeper; b) using a separate low voltage power supply for the hollow cathode keeper; c) using a discharge power supply connected to the keeper through a high-resistance resistor to the hollow cathode keeper; d) connecting the keeper of the hollow cathode to the discharge power supply through an electronic switch with the possibility of adjusting the duration of the keeper connection to the discharge power supply. The graphs of changes in the thrusterβs currents and voltages for various power supply circuits of the hollow cathode keeper are presented. The results of the choice of the start sequence diagram for the Hall engine ST-25 and the experimental studies carried out have shown that the use of an electronic switch with a steep pulse front makes it possible to obtain a reliable thruster start-up when a separate power supply for the keeper is excluded from the power processing unit of the propulsion system. As a result of the work carried out, it became possible to place the power processing unit for a propulsion system based on the ST-25 thruster in a volume of 2U. The possibility of using ST-25 thruster on spacecraft, the onboard electrical power of which is limited up to 200 W were confirmed.ΠΠ°Π²Π΅Π΄Π΅Π½ΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π²ΠΈΠ±ΠΎΡΡ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΈ Π·Π°ΠΏΡΡΠΊΡ ΡΠ° Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΈΡ
Π²ΠΈΠΏΡΠΎΠ±ΡΠ²Π°Π½Ρ Π₯ΠΎΠ»Π»ΠΎΠ²ΡΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³ΡΠ½Π° ST-25, ΠΏΡΠΈΠ·Π½Π°ΡΠ΅Π½ΠΎΠ³ΠΎ Π΄Π»Ρ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½Ρ Π½Π° ΠΌΠ°Π»ΠΈΡ
ΠΊΠΎΡΠΌΡΡΠ½ΠΈΡ
Π°ΠΏΠ°ΡΠ°ΡΠ°Ρ
. Π ΠΌΠ΅ΡΠΎΡ Π·Π½ΠΈΠΆΠ΅Π½Π½Ρ ΠΌΠ°ΡΠΈ ΡΠ° Π³Π°Π±Π°ΡΠΈΡΡΠ² ΡΠΈΡΡΠ΅ΠΌΠΈ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½Π½Ρ Π΅Π½Π΅ΡΠ³ΡΡ Π΄Π²ΠΈΠ³ΡΠ½Π½ΠΎΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Π·Ρ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΡ ΡΡ
Π΅ΠΌΠΈ ΡΠΈΡΡΠ΅ΠΌΠΈ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½Π½Ρ Π΅Π½Π΅ΡΠ³ΡΡ Π·Π°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎ Π²ΠΈΠΊΠ»ΡΡΠΈΡΠΈ Π΄ΠΆΠ΅ΡΠ΅Π»ΠΎ Π΅Π»Π΅ΠΊΡΡΠΎΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ. ΠΠΈΠΊΠ»ΡΡΠ΅Π½Π½Ρ Π΄ΠΆΠ΅ΡΠ΅Π»Π° Π΅Π»Π΅ΠΊΡΡΠΎΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ Π·Ρ ΡΠΊΠ»Π°Π΄Ρ ΡΠΈΡΡΠ΅ΠΌΠΈ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½Π½Ρ Π΅Π½Π΅ΡΠ³ΡΡ Π²ΠΈΠΊΠ»ΠΈΠΊΠ°Π»ΠΎ Π½Π΅ΠΎΠ±Ρ
ΡΠ΄Π½ΡΡΡΡ Π·Π΄ΡΠΉΡΠ½ΠΈΡΠΈ Π²ΠΈΠ±ΡΡ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΈ Π·Π°ΠΏΡΡΠΊΡ Π΄Π²ΠΈΠ³ΡΠ½Π°. Π ΠΎΠ·Π³Π»ΡΠ½ΡΡΠΎ ΡΠΎΡΠΈΡΠΈ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΈ Π·Π°ΠΏΡΡΠΊΡ Π₯ΠΎΠ»Π»ΠΎΠ²ΡΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³ΡΠ½Π° ST-25: Π°) Π· Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½ΡΠΌ Π²ΠΈΡΠΎΠΊΠΎΠ²ΠΎΠ»ΡΡΠ½ΠΎΠ³ΠΎ Π΄ΠΆΠ΅ΡΠ΅Π»Π° Π΅Π»Π΅ΠΊΡΡΠΎΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ; Π±) Π· Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½ΡΠΌ Π½ΠΈΠ·ΡΠΊΠΎΠ²ΠΎΠ»ΡΡΠ½ΠΎΠ³ΠΎ Π΄ΠΆΠ΅ΡΠ΅Π»Π° Π΅Π»Π΅ΠΊΡΡΠΎΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ; Π²) Π· Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½ΡΠΌ Π΄Π»Ρ ΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ Π΄ΠΆΠ΅ΡΠ΅Π»Π° ΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΡΠΎΠ·ΡΡΠ΄Ρ, ΠΏΡΠ΄ΠΊΠ»ΡΡΠ΅Π½ΠΎΠ³ΠΎ Π΄ΠΎ ΠΊΡΠΏΠ΅ΡΡ ΡΠ΅ΡΠ΅Π· Π²ΠΈΡΠΎΠΊΠΎΠΎΠΌΠ½ΠΈΠΉ ΡΠ΅Π·ΠΈΡΡΠΎΡ; Π³) ΠΏΡΠ΄ΠΊΠ»ΡΡΠ΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ Π΄ΠΎ Π΄ΠΆΠ΅ΡΠ΅Π»Π° ΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΡΠΎΠ·ΡΡΠ΄Ρ ΡΠ΅ΡΠ΅Π· Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΈΠΉ ΠΊΠ»ΡΡ Π· ΠΌΠΎΠΆΠ»ΠΈΠ²ΡΡΡΡ ΡΠ΅Π³ΡΠ»ΡΠ²Π°Π½Π½Ρ ΡΠ°ΡΡ ΠΏΡΠ΄ΠΊΠ»ΡΡΠ΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ Π΄ΠΎ Π΄ΠΆΠ΅ΡΠ΅Π»Π° ΡΠΎΠ·ΡΡΠ΄Ρ. ΠΠ°Π²Π΅Π΄Π΅Π½ΠΎ Π³ΡΠ°ΡΡΠΊΠΈ Π·ΠΌΡΠ½ΠΈ ΡΡΡΡΠΌΡΠ² ΡΠ° Π½Π°ΠΏΡΡΠ³ Π΄Π²ΠΈΠ³ΡΠ½Π° Π΄Π»Ρ ΡΡΠ·Π½ΠΈΡ
ΡΡ
Π΅ΠΌ Π΅Π»Π΅ΠΊΡΡΠΎΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π²ΠΈΠ±ΠΎΡΡ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΈ Π·Π°ΠΏΡΡΠΊΡ Π₯ΠΎΠ»Π»ΠΎΠ²ΡΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³ΡΠ½Π° ST-25 ΡΠ° ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Ρ Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Ρ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΠΎ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½Ρ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΡΡΠ° Π· ΠΊΡΡΡΠΈΠΌ ΡΡΠΎΠ½ΡΠΎΠΌ ΡΠΌΠΏΡΠ»ΡΡΡ Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡ Π·Π°Π±Π΅Π·ΠΏΠ΅ΡΠΈΡΠΈ Π½Π°Π΄ΡΠΉΠ½ΠΈΠΉ Π·Π°ΠΏΡΡΠΊ Π΄Π²ΠΈΠ³ΡΠ½Π° ΠΏΡΠΈ Π²ΠΈΠΊΠ»ΡΡΠ΅Π½Π½Ρ Π·Ρ ΡΠΊΠ»Π°Π΄Ρ ΡΠΈΡΡΠ΅ΠΌΠΈ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½Π½Ρ Π΅Π½Π΅ΡΠ³ΡΡ Π΄Π²ΠΈΠ³ΡΠ½Π½ΠΎΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΎΠΊΡΠ΅ΠΌΠΎΠ³ΠΎ Π΄ΠΆΠ΅ΡΠ΅Π»Π° ΠΆΠΈΠ²Π»Π΅Π½Π½Ρ ΠΊΡΠΏΠ΅ΡΡ. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ
Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Ρ Π²ΠΈΡΠ²ΠΈΠ»ΠΎΡΡ ΠΌΠΎΠΆΠ»ΠΈΠ²ΠΈΠΌ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½Π½Ρ Π΅Π½Π΅ΡΠ³ΡΡ Π΄Π»Ρ Π΄Π²ΠΈΠ³ΡΠ½Π½ΠΎΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Π½Π° Π±Π°Π·Ρ Π΄Π²ΠΈΠ³ΡΠ½Π° ST-25 ΡΠΎΠ·ΠΌΡΡΡΠΈΡΠΈ Ρ ΠΎΠ±βΡΠΌΡ 2U. ΠΡΠ΄ΡΠ²Π΅ΡΠ΄ΠΆΠ΅Π½ΠΎ ΠΌΠΎΠΆΠ»ΠΈΠ²ΡΡΡΡ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½Ρ Π΄Π²ΠΈΠ³ΡΠ½ΡΠ² ST-25 Π½Π° ΠΊΠΎΡΠΌΡΡΠ½ΠΈΡ
Π°ΠΏΠ°ΡΠ°ΡΠ°Ρ
, Π±ΠΎΡΡΠΎΠ²Π° Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½Π° ΠΏΠΎΡΡΠΆΠ½ΡΡΡΡ ΡΠΊΠΈΡ
ΠΎΠ±ΠΌΠ΅ΠΆΠ΅Π½Π° Π²Π΅Π»ΠΈΡΠΈΠ½ΠΎΡ 200 ΠΡ.ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π²ΡΠ±ΠΎΡΠ° ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΌΡ Π·Π°ΠΏΡΡΠΊΠ° ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ Π₯ΠΎΠ»Π»ΠΎΠ²ΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ ST-25, ΠΏΡΠ΅Π΄Π½Π°Π·Π½Π°ΡΠ΅Π½Π½ΠΎΠ³ΠΎ Π΄Π»Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π½Π° ΠΌΠ°Π»ΡΡ
ΠΊΠΎΡΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Π°ΠΏΠΏΠ°ΡΠ°ΡΠ°Ρ
. Π‘ ΡΠ΅Π»ΡΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΌΠ°ΡΡΡ ΠΈ Π³Π°Π±Π°ΡΠΈΡΠΎΠ² ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΈΠ· ΡΡΡΡΠΊΡΡΡΡ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΎ ΠΈΡΠΊΠ»ΡΡΠΈΡΡ ΠΈΡΡΠΎΡΠ½ΠΈΠΊ ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π°. ΠΡΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΈΠ· ΡΠΎΡΡΠ°Π²Π° ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π²ΡΠ·Π²Π°Π»ΠΎ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΠΎΡΡΡΠ΅ΡΡΠ²ΠΈΡΡ Π²ΡΠ±ΠΎΡ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΌΡ Π·Π°ΠΏΡΡΠΊΠ° Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ. Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΡΠ΅ΡΡΡΠ΅ ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΌΡ Π·Π°ΠΏΡΡΠΊΠ° Π₯ΠΎΠ»Π»ΠΎΠ²ΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ ST-25: Π°) Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π²ΡΡΠΎΠΊΠΎΠ²ΠΎΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π°; Π±) Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π½ΠΈΠ·ΠΊΠΎΠ²ΠΎΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π°; Π²) Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π΄Π»Ρ ΠΏΠΈΡΠ°Π½ΠΈΡ ΡΠ΅ΠΏΠ΅ΠΉ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π° ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΡΠ°Π·ΡΡΠ΄Π°, ΠΏΠΎΠ΄ΠΊΠ»ΡΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΊ ΠΊΠΈΠΏΠ΅ΡΡ ΡΠ΅ΡΠ΅Π· Π²ΡΡΠΎΠΊΠΎΠΎΠΌΠ½ΡΠΉ ΡΠ΅Π·ΠΈΡΡΠΎΡ; Π³) ΠΏΠΎΠ΄ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π° ΠΊ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΡ ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΡΠ°Π·ΡΡΠ΄Π° ΡΠ΅ΡΠ΅Π· ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠΉ ΠΊΠ»ΡΡ Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡΡ ΡΠ΅Π³ΡΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΏΠΎΠ΄ΠΊΠ»ΡΡΠ΅Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΊ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΡ ΡΠ°Π·ΡΡΠ΄Π°. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ Π³ΡΠ°ΡΠΈΠΊΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠΎΠΊΠΎΠ² ΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ Π΄Π»Ρ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΡΡ
ΡΡ
Π΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°ΡΠΎΠ΄Π°. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ Π²ΡΠ±ΠΎΡΠ° ΡΠΈΠΊΠ»ΠΎΠ³ΡΠ°ΠΌΠΌΡ Π·Π°ΠΏΡΡΠΊΠ° Π₯ΠΎΠ»Π»ΠΎΠ²ΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ ST-25 ΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΠ΅ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΡΡΠ° Ρ ΠΊΡΡΡΡΠΌΠΈ ΡΡΠΎΠ½ΡΠ°ΠΌΠΈ ΠΈΠΌΠΏΡΠ»ΡΡΠ° ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΡΡ Π½Π°Π΄Π΅ΠΆΠ½ΡΠΉ Π·Π°ΠΏΡΡΠΊ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ ΠΏΡΠΈ ΠΈΡΠΊΠ»ΡΡΠ΅Π½ΠΈΠΈ ΠΈΠ· ΡΠΎΡΡΠ°Π²Π° ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΎΡΠ΄Π΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΊΠΈΠΏΠ΅ΡΠ°. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΡ
ΡΠ°Π±ΠΎΡ ΠΎΠΊΠ°Π·Π°Π»ΠΎΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠΌ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π΄Π»Ρ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Π½Π° Π±Π°Π·Π΅ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Ρ ST-25 ΡΠ°Π·ΠΌΠ΅ΡΡΠΈΡΡ Π² ΠΎΠ±ΡΠ΅ΠΌΠ΅ 2U. ΠΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»Π΅ΠΉ ST-25 Π½Π° ΠΊΠΎΡΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Π°ΠΏΠΏΠ°ΡΠ°ΡΠ°Ρ
, Π±ΠΎΡΡΠΎΠ²Π°Ρ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠΎΡΠ½ΠΎΡΡΡ ΠΊΠΎΡΠΎΡΡΡ
ΠΎΠ³ΡΠ°Π½ΠΈΡΠ΅Π½Π° Π²Π΅Π»ΠΈΡΠΈΠ½ΠΎΠΉ 200 ΠΡ
Three-dimensional investigation of liquid film structure at the initial area of annular-dispersed flow
Initial stage of downward flow of gas-sheared liquid film in a vertical rectangular duct was studied using brightness-based laser-induced fluorescence technique. Measurements were resolved along both longitudinal and transverse coordinates and time. The initial high-frequency waves which are formed at the inlet were found to be two-dimensional. These waves are promptly broken into localised horseshoe-shaped waves which merge downstream to form large-scale quasi-2D disturbance waves. Peculiarities of three-dimensional evolution of waves of different types were studied in a wide range of flow parameters
Three-dimensional investigation of liquid film structure at the initial area of annular-dispersed flow
Initial stage of downward flow of gas-sheared liquid film in a vertical rectangular duct was studied using brightness-based laser-induced fluorescence technique. Measurements were resolved along both longitudinal and transverse coordinates and time. The initial high-frequency waves which are formed at the inlet were found to be two-dimensional. These waves are promptly broken into localised horseshoe-shaped waves which merge downstream to form large-scale quasi-2D disturbance waves. Peculiarities of three-dimensional evolution of waves of different types were studied in a wide range of flow parameters
UAV-Derived Data Application for Environmental Monitoring of the Coastal Area of Lake Sevan, Armenia with a Changing Water Level
The paper presents the range and applications of thematic tasks for ultra-high spatial resolution data from small unmanned aerial vehicles (UAVs) in the integral system of environmental multi-platform and multi-scaled monitoring of Lake Sevan, which is one of the greatest freshwater lakes in Eurasia. From the 1930s, it had been subjected to human-driven changing of the water level with associated and currently exacerbated environmental issues. We elaborated the specific techniques of optical and thermal surveys for the different coastal sites and phenomena in study. UAV-derived optical imagery and thermal stream were processed by a Structure-from-Motion algorithm to create digital surface models (DSMs) and ortho-imagery for several key sites. UAV imagery were used as additional sources of detailed spatial data under large-scale mapping of current land-use and point sources of water pollution in the coastal zone, and a main data source on environmental violations, especially sewage discharge or illegal landfills. The revealed present-day coastal types were mapped at a large scale, and the net changes of shoreline position and rates of shore erosion were calculated on multi-temporal UAV data using modified Hausdorff’s distance. Based on highly-detailed DSMs, we revealed the areas and objects at risk of flooding under the projected water level rise to 1903.5 m along the west coasts of Minor Sevan being the most popular recreational area. We indicated that the structural and environmental state of marsh coasts and coastal wetlands as potential sources of lake eutrophication and associated algal blooms could be more efficiently studied under thermal UAV surveys than optical ones. We proposed to consider UAV surveys as a necessary intermediary between ground data and satellite imagery with different spatial resolutions for the complex environmental monitoring of the coastal area and water body of Lake Sevan as a whole
Experimental study of air delivery into water-conveyance system of the radial-axial turbine
The paper presents an experimental study of oscillatory response in the Francis turbine of hydraulic unit. The experiment was performed on large-scale hydrodynamic test-bench with impeller diameter of 0.3 m. The effect of air injection on the intensity of pressure pulsations was studied at the maximum pressure pulsations in the hydraulic unit. It was revealed that air delivery into the water-conveyance system of the turbine results in almost two-fold reduction of pressure pulsations