Zobrazeno 1 - 7
of 7
pro vyhledávání: '"Branko R. Obrović"'
Publikováno v:
Thermal Science, Vol 17, Iss 2, Pp 555-566 (2013)
This paper studies the ionized gas i.e. air flow in an axisymmetrical boundary layer adjacent to the bodies of revolution. The contour of the body within the fluid is nonporous. The ionized gas flows under the conditions of equilibrium ionization. A
Publikováno v:
Thermal Science. 14:183-196
This paper studies the influence of the magnetic field on the planar laminar steady flow of the ionized gas in the boundary layer. The present outer magnetic field is homogenous and perpendicular to the body within the fluid. The gas of the same phys
Publikováno v:
Thermal Science, Vol 14, Iss 5, Pp 183-196 (2010)
THE INFLUENCE OF THE MAGNETIC FIELD ON THE IONIZED GAS FLOW ADJACENT TO THE POROUS WALL
Publikováno v:
Theoretical and Applied Mechanics, Vol 36, Iss 2, Pp 119-135 (2009)
This paper concerns with unsteady two-dimensional temperature laminar magnetohydrodynamic (MHD) boundary layer of incompressible fluid. It is assumed that induction of outer magnetic field is function of longitudinal coordinate with force lines perpe
Autor:
Branko R. Obrović, Slobodan Savić
Publikováno v:
Theoretical and Applied Mechanics, Vol 33, Iss 2, Pp 149-179 (2006)
This paper investigates ionized gas flow in the boundary layer when its electroconductivity is varied. The flow is planar and the contour is porous. At first, it is assumed that the ionized gas electroconductivity ? depends only on the longitudinal v
Publikováno v:
Theoretical and Applied Mechanics, Vol 32, Iss 2, Pp 165-190 (2005)
This paper studies the ideally dissociated air flow in the boundary layer when the contour of the body within the fluid is porous. By means of adequate transformations, the governing boundary layer equations of the problem are brought to a general fo
Publikováno v:
Tehnički vjesnik
Volume 17
Issue 1
Volume 17
Issue 1
This paper studies ionized gas flow in the boundary layer on bodies of revolution. The present magnetic field is normal to a nonporous contour of the body. The governing boundary layer equations are brought to a generalized form by general similarity