Ionized gas boundary layer on a porous wall of the body within the electroconductive fluid | Zendy

Branko Obrovic | Zendy; Slobodan Savić | Zendy

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Ionized gas boundary layer on a porous wall of the body within the electroconductive fluid

Author(s) -

Branko Obrovic,

Slobodan Savić

Publication year - 2004

Publication title -

theoretical and applied mechanics

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.279

H-Index - 6

eISSN - 2406-0925

pISSN - 1450-5584

DOI - 10.2298/tam0401047o

Subject(s) - boundary layer , ionization , plasma , blasius boundary layer , boundary (topology) , mechanics , perpendicular , layer (electronics) , boundary layer thickness , boundary value problem , magnetic field , flow (mathematics) , materials science , porosity , physics , geometry , classical mechanics , mathematical analysis , mathematics , composite material , ion , quantum mechanics

This paper investigates the ionized gas flow in the boundary layer, when the contour of the body within the fluid is porous. Ionized gas is exposed to the influence of the outer magnetic field induction Bm = Bm(x), which is perpendicular to the contour of the body within the fluid. It is presumed that the electroconductivity of the ionized gas is a function only of the longitudinal coordinate, i.e. ¾ = ¾(x). By means of adequate transformations, the governing boundary layer equations are brought to a generalized form. The obtained generalized equations are solved in a four-parameter localized approximation. Based on the obtained numerical solutions, diagrams of important physical values and characteristics of the boundary layer have been made. Conclusions have also been drawn

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