{"id":2998,"date":"2023-05-23T13:25:13","date_gmt":"2023-05-23T10:25:13","guid":{"rendered":"http:\/\/itm.dp.ua\/?page_id=2998"},"modified":"2023-05-23T13:29:22","modified_gmt":"2023-05-23T10:29:22","slug":"plasma-gas-dynamic-plant-plasmoelectrodynamic-bench","status":"publish","type":"page","link":"http:\/\/itm.dp.ua\/?page_id=2998&lang=en","title":{"rendered":"Plasma gas-dynamic plant (plasmoelectrodynamic bench)"},"content":{"rendered":"\n<p>Department of ionized media mechanics<\/p>\n\n\n\n<p>Head of department &#8211; D.Sc., Professor\u00a0<a href=\"http:\/\/itm.dp.ua\/?page_id=1186&amp;lang=en\" data-type=\"page\" data-id=\"1186\">V. O. Shuvalov<\/a><\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img decoding=\"async\" src=\"http:\/\/itm.dp.ua\/wp-content\/uploads\/2023\/05\/Otd4_1-768x408.jpg\" alt=\"\"\/><figcaption class=\"wp-element-caption\">Plasma gas-dynamic plant (plasmoelectrodynamic bench)<\/figcaption><\/figure>\n\n\n\n<p><strong>Key specifications<\/strong><\/p>\n\n\n\n<p>The bench is a plasma gas-dynamic tunnel.The 100 m\u00b3\/s evacuation system of the bench and its cryopanels cooled with liquid nitrogen produce a static vacuum of 10-5 N\/m2\u00b2 in the work chamber, which is a nonmagnetic steel cylinder of diameter 1.2 m and length 3.5 m \u2014 with gas inleakage, the chamber pressure is 10<sup>-4<\/sup>&nbsp;\u2014 10<sup>-2<\/sup>&nbsp;N\/m2. Supersonic rarefied plasma flows are produced using a hot-cathode gas-discharge accelerator, whose working medium is ionized by electron impact and electron oscillation in an external magnetic field. The plasma flow parameters are measured using a system of electrical and pressure probes, 5.45 and 9.8 GHz interferometers, and a \u041c\u04257303 mass-spectrometer. The diagnostic instruments and models under study are placed on the movable platforms of the upper and lower coordinate tables with four degrees of freedom each. The positioning is checked using potentiometric pickups. The positioning accuracy is \u2014 0.5 \u00b7 10<sup>-3<\/sup>&nbsp;m for linear displacements and \u2014 0.5 \u00b0 for angular ones.<\/p>\n\n\n\n<p><strong>Description<\/strong><\/p>\n\n\n\n<p>The plasmoelectrodynamic bench serves to study various aspects of interaction between a solid body (e.g. spacecraft materials and structural elements) with its environment in the Earth ionosphere and magnetosphere. The bench systems and capabilities allow one to simulate the interaction of the planets of the Solar System, artificial bodies, and spacecraft with the interplanetary medium (solar wind), cold ionospheric and hot magnetospheric plasma flows, charged-particle streams, electric and magnetic fields, and solar-spectrum and radar-range electromagnetic radiation in high-elliptical, geostationary, low, medium, and geopolar orbits at altitudes of 150 to 40,000 km.<\/p>\n\n\n\n<p>The plasmoelectrodynamic bench is the National Treasure according to the Cabinet of Ministers of Ukraine&#8217;s order #650 from 28\/08\/2013.<\/p>\n\n\n\n<p><strong>Capabilities<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>contact diagnostics of the neutral and charged components of high-speed flows of nonequilibrium collisional and collisionless partially dissociated plasma in the pressure range 10<sup>3<\/sup>\u00a0down to 10<sup>-9<\/sup><\/li>\n\n\n\n<li>study of the acceleration mechanisms and flow pattern for plasma bunches and steady and pulse plasma jets expanding into vacuum; revealing the effects and mechanisms of attenuation and distortion of radio signals reflected from spacecraft elements in the centimetric, decimetric and metric wave bands by the plasma jets and artificial plasma formations produced in the vicinity of the spacecraft surface as a result of the operation of electrojet engines, electron beam injection, and passive and active in-orbit experiments;<\/li>\n\n\n\n<li>simulation and study of the processes, mechanisms, and regularities of accumulation and neutralization of high-voltage charges during the exposure of dielectric materials and spacecraft surface coatings to electromagnetic radiation and high-energy electrons of the Earth radiation belts in a geostationary orbit and to auroral electrons when the spacecraft is in a supersonic flow of cold plasma in the polar ionosphere;<\/li>\n\n\n\n<li>physical-chemical simulation and study of solar battery power degradation and the behavior of the weight, geometrical, and thermooptical characteristics of solar battery polymer and composite materials during long-term exposure to a complex of space factors in a geostationary orbit and to a supersonic flow of atomic oxygen and ultraviolet radiation in the Earth atmosphere;<\/li>\n\n\n\n<li>physical simulation of the effects and regularities of magneto-hydrodynamic interaction of magnetized bodies with a rarefied plasma flow;<\/li>\n\n\n\n<li>aerodynamics and heat exchange of spacecraft and their structural elements in a rarified plasma flow.<\/li>\n<\/ul>\n\n\n\n<p><strong>Comparison with existing analogs<\/strong><\/p>\n\n\n\n<p>The plasmoelectrodynamic bench combines the features of a plasma gas-dynamic tunnel, an electroradiation bench, and a vacuum anechioc chamber. In this sum of features and the range of scientific and tecnical problems it solves, the bench is unparalleled.<\/p>\n\n\n\n<p>The punblished results of investigations illustrate the capabilities of the plasmoelectrodynamic bench:<\/p>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Shuvalov V. A. Structure of bunches and jets of a plasma pulse expanding into vacuum (in Russian) \/ V. A. Shuvalov, M. G. Bystritskii, G. S. Kochubei, A. E. Churilov \/\/ Teplofizika Vysokikh Temperatur. \u2013 2004. \u2013 N. 42, No 1. \u2013 Pp. 23 &#8211; 30.<\/li>\n\n\n\n<li>Shuvalov V. A. Molecular contamination of the spacecraft surface in thermostating and orbital injection (in Russian) \/ Shuvalov V. A., Tikhii V. G., Potapovich L. P., Priimak A. I., Pismennyi N. I., Kochubei G. S. \/\/ Kosmichna Nauka i Tekhnologiya. \u2013 2007. \u2013 V. 13, No 3. \u2013 Pp. 3 \u2013 11.<\/li>\n\n\n\n<li>Shuvalov V. A. Probe diagnostics of high-speed flows of partially dissociated rarefied plasma (in Russian) \/ V.A. Shuvalov, N. I. Pismennyi, A. I. Priimak, G. S. Kochubei \/\/ Pribory i Tekhnika Eksperimenta. \u2013 2007. \u2013 No 2. \u2013 Pp. 92 \u2013 100.<\/li>\n\n\n\n<li>Shuvalov V. A. Behavior of spacecraft solar panel materials exposed to atomic oxygen (in Russian) \/ V. A. Shuvalov, G. S. Kochubei, A. I. Priimak, N. I. Pismennyi , N. A. Tokmak \/\/ Kosmicheskie Issledovaniya. \u2013 2007. \u2013 V. 45, No 4. \u2013 Pp. 294 \u2013 304.<\/li>\n\n\n\n<li>Shuvalov V. A. Magnetodynamic braking of the \u201cmagnetized\u201d planets in a solar wind plasma flow (in Russian) \/ Shuvalov V.A. Bandel K. A., Priimak A. I., Kochubei G. S. \/\/ Kosmichna Nauka i Tekhnologiya. \u2013 2009. \u2013 V. 15, No 6. \u2013 Pp. 3 -13.<\/li>\n\n\n\n<li>Pismennyi N. Physical modeling of interaction of spacecraft with near-satellite environment \/ Pismennyi N., Priimak A., Nosikov S., Tsokur A. \/\/ Space Research in Ukraine 2006 \u2013 2008 \/ National Space Agency of Ukraine. \u2013 Kiev, 2008. \u2013 Pp. 101\u2013 106.<\/li>\n\n\n\n<li>Shuvalov V. A. Charge transfer by fast electrons onto the leeward surfaces of a solid body in a supersonic rarefied plasma flow (in Russian) \/ Shuvalov V. A., Priimak A. I., Bandel K. A., Kochubei G. S. \/\/ Prikladnaya Mekhanika i Tekhnicheskaya Fizika. \u2013 2008. \u2013 V. 49, No 1. \u2013 Pp. 13 \u2013 23.<\/li>\n\n\n\n<li>Shuvalov V. A. Diagnostics of the neutral and the charged component of a rarefied plasma flow with calorimetric probes (in Russian) \/ V. A. Shuvalov, D. N. Lazuchenkov, G. S. Kochubei, S. V. Nosikov \/\/ Pribory i Tekhnika Eksperimenta. \u2013 2010. \u2013 No 3. \u2013 Pp. 80 \u2013 87.<\/li>\n\n\n\n<li>Shuvalov V. A. Diagnostics of nonequilibrium collisional plasma with a hot-wire anemometer probe (in Russian) \/ V. A. Shuvalov, G. S. Kochubei, D. N. Lazuchenkov \/\/ Teplofizika Vysokikh Temperatur. \u2013 2011. \u2013 V. 48, No 1. \u2013 Pp. 28 \u2013 35.<\/li>\n\n\n\n<li>Shuvalov V. A. Control of the heat exchange and braking of a \u201cmagnetized\u201d body in a rarefied plasma flow (in Russian) \/ V. A. Shuvalov, A. I. Priimak, K. A. Bandel, G. S. Kochubei, N. A. Tokmak \/\/ Teplofizika Vysokikh Temperatur.. \u2013 2011. \u2013 V. 48, No 3. \u2013 Pp. 1-10.<\/li>\n\n\n\n<li>Shuvalov V. A. Heat exchange and braking of a \u201cmagnetized\u201d body in a rarefied plasma flow (in Russian) \/ V. A. Shuvalov, A. I. Priimak, K. A. Bandel, G. S. Kochubei, N. A. Tokmak \/\/ Prikladnaya Mekhanika i Tekhnicheskaya Fizika. \u2013 2011. \u2013 V. 52, No 1. \u2013 Pp. 1 \u2013 14.<\/li>\n<\/ol>\n","protected":false},"excerpt":{"rendered":"<p>Department of ionized media mechanics Head of department &#8211; D.Sc., Professor\u00a0V. O. Shuvalov Key specifications The bench is a plasma gas-dynamic tunnel.The 100 m\u00b3\/s evacuation system of the bench and&hellip;<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-2998","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/pages\/2998","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/itm.dp.ua\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=2998"}],"version-history":[{"count":3,"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/pages\/2998\/revisions"}],"predecessor-version":[{"id":3002,"href":"http:\/\/itm.dp.ua\/index.php?rest_route=\/wp\/v2\/pages\/2998\/revisions\/3002"}],"wp:attachment":[{"href":"http:\/\/itm.dp.ua\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=2998"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}