Отрывок: For spatial discretization of density, momentum, energy and turbulent quantities, a second-order upwind scheme is applied. The program package solves governing equations using the finite volumes method. The computational grids consisted of about 4 106 hexahedral cells. Three different types of electrodes are considered in the simulation: a thick electrode, a thin electrode, and a pipe-like electrode. Largely, the structure of the flow is determined by the paraxial counterflow zone...
Полная запись метаданных
Поле DC | Значение | Язык |
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dc.contributor.author | Klimov, A.I. | - |
dc.contributor.author | Kurushina, S.E. | - |
dc.contributor.author | Molevich, N.E. | - |
dc.contributor.author | Porfiriev, D.P. | - |
dc.contributor.author | Zavershinskii, I.P. | - |
dc.date.accessioned | 2018-08-14 15:23:15 | - |
dc.date.available | 2018-08-14 15:23:15 | - |
dc.date.issued | 2018 | - |
dc.identifier | Dspace\SGAU\20180813\71385 | ru |
dc.identifier.citation | Klimov A.I. Plasma vortex reactor for production of heat energy and hydrogen / A.I. Klimov, S.E. Kurushina, N.E. Molevich, D.P. Porfiriev, I.P. Zavershinskii // International Conference on Combustion Physics and Chemistry // (Samara, Russia, 24-28 July): proceeding of the conference / Samara University; Edited by A.M. Mebel and V.N. Azyazov – Samara: Publishing OOO “Insoma-Press”, 2018 – p. 112 | ru |
dc.identifier.isbn | 978-5-4317-0298-3 | - |
dc.identifier.uri | http://repo.ssau.ru/handle/International-Conference-on-Combustion-Physics-and-Chemistry/Plasma-vortex-reactor-for-production-of-heat-energy-and-hydrogen-71385 | - |
dc.language.iso | en | ru |
dc.publisher | Publishing OOO “Insoma-Press” | ru |
dc.title | Plasma vortex reactor for production of heat energy and hydrogen | ru |
dc.type | Thesis | ru |
dc.textpart | For spatial discretization of density, momentum, energy and turbulent quantities, a second-order upwind scheme is applied. The program package solves governing equations using the finite volumes method. The computational grids consisted of about 4 106 hexahedral cells. Three different types of electrodes are considered in the simulation: a thick electrode, a thin electrode, and a pipe-like electrode. Largely, the structure of the flow is determined by the paraxial counterflow zone... | - |
Располагается в коллекциях: | International Conference on Combustion Physics and Chemistry |
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