31 research outputs found

    Improved Modeling of Peptide-Protein Binding Through Global Docking and Accelerated Molecular Dynamics Simulations

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    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 3.3–4.8 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 0.6–2.7 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

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    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

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    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 (70–75%) 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 70–80% 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

    Therapeutic properties of a vector carrying the HSV thymidine kinase and GM-CSF genes and delivered as a complex with a cationic copolymer

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    Π¦Π˜ΠšΠ›ΠžΠ“Π ΠΠœΠœΠ« Π—ΠΠŸΠ£Π‘ΠšΠ Π₯ΠžΠ›Π›ΠžΠ’Π‘ΠšΠžΠ“Πž Π”Π’Π˜Π“ΠΠ’Π•Π›Π― ST-25

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    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 thruster’s 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.НавСдСно Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π²ΠΈΠ±ΠΎΡ€Ρƒ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΈ запуску Ρ‚Π° Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΈΡ… Π²ΠΈΠΏΡ€ΠΎΠ±ΡƒΠ²Π°Π½ΡŒ Π₯олловського Π΄Π²ΠΈΠ³ΡƒΠ½Π° ST-25, ΠΏΡ€ΠΈΠ·Π½Π°Ρ‡Π΅Π½ΠΎΠ³ΠΎ для використання Π½Π° ΠΌΠ°Π»ΠΈΡ… космічних Π°ΠΏΠ°Ρ€Π°Ρ‚Π°Ρ…. Π— ΠΌΠ΅Ρ‚ΠΎΡŽ зниТСння маси Ρ‚Π° Π³Π°Π±Π°Ρ€ΠΈΡ‚Ρ–Π² систСми пСрСтворСння Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π΄Π²ΠΈΠ³ΡƒΠ½Π½ΠΎΡ— установки Π·Ρ– структурної схСми систСми пСрСтворСння Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π·Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎ Π²ΠΈΠΊΠ»ΡŽΡ‡ΠΈΡ‚ΠΈ Π΄ΠΆΠ΅Ρ€Π΅Π»ΠΎ СлСктроТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ. Π’ΠΈΠΊΠ»ΡŽΡ‡Π΅Π½Π½Ρ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° СлСктроТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ Π·Ρ– складу систСми пСрСтворСння Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π²ΠΈΠΊΠ»ΠΈΠΊΠ°Π»ΠΎ Π½Π΅ΠΎΠ±Ρ…Ρ–Π΄Π½Ρ–ΡΡ‚ΡŒ здійснити Π²ΠΈΠ±Ρ–Ρ€ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΈ запуску Π΄Π²ΠΈΠ³ΡƒΠ½Π°. Розглянуто Ρ‡ΠΎΡ‚ΠΈΡ€ΠΈ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΈ запуску Π₯олловського Π΄Π²ΠΈΠ³ΡƒΠ½Π° ST-25: Π°) Π· використанням Π²ΠΈΡΠΎΠΊΠΎΠ²ΠΎΠ»ΡŒΡ‚Π½ΠΎΠ³ΠΎ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° СлСктроТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ; Π±) Π· використанням Π½ΠΈΠ·ΡŒΠΊΠΎΠ²ΠΎΠ»ΡŒΡ‚Π½ΠΎΠ³ΠΎ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° СлСктроТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ; Π²) Π· використанням для ТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° ТивлСння розряду, ΠΏΡ–Π΄ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΎΠ³ΠΎ Π΄ΠΎ ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ Ρ‡Π΅Ρ€Π΅Π· високоомний рСзистор; Π³) ΠΏΡ–Π΄ΠΊΠ»ΡŽΡ‡Π΅Π½Π½Ρ ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ Π΄ΠΎ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° ТивлСння розряду Ρ‡Π΅Ρ€Π΅Π· Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΈΠΉ ΠΊΠ»ΡŽΡ‡ Π· ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŽ Ρ€Π΅Π³ΡƒΠ»ΡŽΠ²Π°Π½Π½Ρ часу ΠΏΡ–Π΄ΠΊΠ»ΡŽΡ‡Π΅Π½Π½Ρ ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ Π΄ΠΎ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° розряду. НавСдСно Π³Ρ€Π°Ρ„Ρ–ΠΊΠΈ Π·ΠΌΡ–Π½ΠΈ струмів Ρ‚Π° Π½Π°ΠΏΡ€ΡƒΠ³ Π΄Π²ΠΈΠ³ΡƒΠ½Π° для Ρ€Ρ–Π·Π½ΠΈΡ… схСм СлСктроТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Ρƒ. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π²ΠΈΠ±ΠΎΡ€Ρƒ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΈ запуску Π₯олловського Π΄Π²ΠΈΠ³ΡƒΠ½Π° ST-25 Ρ‚Π° ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ– Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ– дослідТСння ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‰ΠΎ використання Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΡŽΡ‡Π° Π· ΠΊΡ€ΡƒΡ‚ΠΈΠΌ Ρ„Ρ€ΠΎΠ½Ρ‚ΠΎΠΌ Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΡƒ дозволяє Π·Π°Π±Π΅Π·ΠΏΠ΅Ρ‡ΠΈΡ‚ΠΈ Π½Π°Π΄Ρ–ΠΉΠ½ΠΈΠΉ запуск Π΄Π²ΠΈΠ³ΡƒΠ½Π° ΠΏΡ€ΠΈ Π²ΠΈΠΊΠ»ΡŽΡ‡Π΅Π½Π½Ρ– Π·Ρ– складу систСми пСрСтворСння Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π΄Π²ΠΈΠ³ΡƒΠ½Π½ΠΎΡ— установки ΠΎΠΊΡ€Π΅ΠΌΠΎΠ³ΠΎ Π΄ΠΆΠ΅Ρ€Π΅Π»Π° ТивлСння ΠΊΡ–ΠΏΠ΅Ρ€Ρƒ. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ– ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ виявилось ΠΌΠΎΠΆΠ»ΠΈΠ²ΠΈΠΌ систСму пСрСтворСння Π΅Π½Π΅Ρ€Π³Ρ–Ρ— для Π΄Π²ΠΈΠ³ΡƒΠ½Π½ΠΎΡ— установки Π½Π° Π±Π°Π·Ρ– Π΄Π²ΠΈΠ³ΡƒΠ½Π° ST-25 розмістити Ρƒ об’ємі 2U. ΠŸΡ–Π΄Ρ‚Π²Π΅Ρ€Π΄ΠΆΠ΅Π½ΠΎ ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŒ використання Π΄Π²ΠΈΠ³ΡƒΠ½Ρ–Π² ST-25 Π½Π° космічних Π°ΠΏΠ°Ρ€Π°Ρ‚Π°Ρ…, Π±ΠΎΡ€Ρ‚ΠΎΠ²Π° Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½Π° ΠΏΠΎΡ‚ΡƒΠΆΠ½Ρ–ΡΡ‚ΡŒ яких ΠΎΠ±ΠΌΠ΅ΠΆΠ΅Π½Π° Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ΠΎΡŽ 200 Π’Ρ‚.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π²Ρ‹Π±ΠΎΡ€Π° Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΌΡ‹ запуска ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… испытаний Π₯олловского двигатСля ST-25, ΠΏΡ€Π΅Π΄Π½Π°Π·Π½Π°Ρ‡Π΅Π½Π½ΠΎΠ³ΠΎ для примСнСния Π½Π° ΠΌΠ°Π»Ρ‹Ρ… космичСских Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π°Ρ…. Π‘ Ρ†Π΅Π»ΡŒΡŽ сниТСния массы ΠΈ Π³Π°Π±Π°Ρ€ΠΈΡ‚ΠΎΠ² систСмы прСобразования энСргии Π΄Π²ΠΈΠ³Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ установки ΠΈΠ· структуры систСмы прСобразования энСргии ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΎ ΠΈΡΠΊΠ»ΡŽΡ‡ΠΈΡ‚ΡŒ источник элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π°. Π˜ΡΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ источника элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΈΠ· состава систСмы прСобразования энСргии Π²Ρ‹Π·Π²Π°Π»ΠΎ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ ΠΎΡΡƒΡ‰Π΅ΡΡ‚Π²ΠΈΡ‚ΡŒ Π²Ρ‹Π±ΠΎΡ€ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΌΡ‹ запуска двигатСля. РассмотрСны Ρ‡Π΅Ρ‚Ρ‹Ρ€Π΅ Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΌΡ‹ запуска Π₯олловского двигатСля ST-25: Π°) с использованиСм Π²Ρ‹ΡΠΎΠΊΠΎΠ²ΠΎΠ»ΡŒΡ‚Π½ΠΎΠ³ΠΎ источника элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π°; Π±) с использованиСм Π½ΠΈΠ·ΠΊΠΎΠ²ΠΎΠ»ΡŒΡ‚Π½ΠΎΠ³ΠΎ источника элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π°; Π²) с использованиСм для питания Ρ†Π΅ΠΏΠ΅ΠΉ ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π° источника элСктропитания разряда, ΠΏΠΎΠ΄ΠΊΠ»ΡŽΡ‡Π΅Π½Π½ΠΎΠ³ΠΎ ΠΊ ΠΊΠΈΠΏΠ΅Ρ€Ρƒ Ρ‡Π΅Ρ€Π΅Π· высокоомный рСзистор; Π³) ΠΏΠΎΠ΄ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π° ΠΊ источнику элСктропитания разряда Ρ‡Π΅Ρ€Π΅Π· элСктронный ΠΊΠ»ΡŽΡ‡ с Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒΡŽ рСгулирования Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΏΠΎΠ΄ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΊ источнику разряда. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Π³Ρ€Π°Ρ„ΠΈΠΊΠΈ измСнСния Ρ‚ΠΎΠΊΠΎΠ² ΠΈ напряТСний двигатСля для ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹Ρ… схСм элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π° ΠΏΠΎΠ»ΠΎΠ³ΠΎ ΠΊΠ°Ρ‚ΠΎΠ΄Π°. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π²Ρ‹Π±ΠΎΡ€Π° Ρ†ΠΈΠΊΠ»ΠΎΠ³Ρ€Π°ΠΌΠΌΡ‹ запуска Π₯олловского двигатСля ST-25 ΠΈ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹Π΅ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ исслСдования ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ элСктронного ΠΊΠ»ΡŽΡ‡Π° с ΠΊΡ€ΡƒΡ‚Ρ‹ΠΌΠΈ Ρ„Ρ€ΠΎΠ½Ρ‚Π°ΠΌΠΈ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ Π½Π°Π΄Π΅ΠΆΠ½Ρ‹ΠΉ запуск двигатСля ΠΏΡ€ΠΈ ΠΈΡΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠΈ ΠΈΠ· состава систСмы прСобразования энСргии Π΄Π²ΠΈΠ³Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ установки ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ источника элСктропитания ΠΊΠΈΠΏΠ΅Ρ€Π°. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹Ρ… Ρ€Π°Π±ΠΎΡ‚ оказалось Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹ΠΌ систСму прСобразования энСргии для Π΄Π²ΠΈΠ³Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ установки Π½Π° Π±Π°Π·Π΅ двигатСля ST-25 Ρ€Π°Π·ΠΌΠ΅ΡΡ‚ΠΈΡ‚ΡŒ Π² объСмС 2U. ΠŸΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ примСнСния Π΄Π²ΠΈΠ³Π°Ρ‚Π΅Π»Π΅ΠΉ ST-25 Π½Π° космичСских Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π°Ρ…, бортовая элСктричСская ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… ΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π΅Π½Π° Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ΠΎΠΉ 200 Π’Ρ‚

    Three-dimensional investigation of liquid film structure at the initial area of annular-dispersed flow

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    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

    No full text
    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

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    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

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    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
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