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E.F.F Botta, D Dijkstra
An improved numerical solution of the Navier‐Stokes equations for laminar flow past a semi‐infinite flat plate
E. Botta, D. Dijkstra, A. Veldman (1972)
The numerical solution of the Navier-Stokes equations for laminar, incompressible flow past a parabolic cylinderJournal of Engineering Mathematics, 6
S. Dennis, J. Walsh (1971)
Numerical solutions for steady symmetric viscous flow past a parabolic cylinder in a uniform streamJournal of Fluid Mechanics, 50
A.M. Maqableh
Flow and heat transfer characteristics for laminar flow over parabolic bodies
A. Vooren, D. Dijkstra (1970)
The Navier-Stokes solution for laminar flow past a semi-infinite flat plateJournal of Engineering Mathematics, 4
O.M Haddad
Numerical study of leading edge receptivity over parabolic bodies
O.M Haddad, Th Corke
Numerical study of leading‐edge receptivity on parabolic bodies to freestream acoustic disturbance
R. Davis (1972)
Numerical solution of the Navier-Stokes equations for symmetric laminar incompressible flow past a parabolaJournal of Fluid Mechanics, 51
H. Schlichting (1955)
Boundary Layer Theory
D. Anderson, J. Tannehill, R. Pletcher (2020)
Computational Fluid Mechanics and Heat Transfer
O. Haddad, T. Corke (1998)
Boundary layer receptivity to free-stream sound on parabolic bodiesJournal of Fluid Mechanics, 368
S.C.R Dennis, J.D Walsh
Numerical solution for steady symmetric flow past a parabolic cylinder in uniform stream flow
R. Davis (1967)
Laminar incompressible flow past a semi-infinite flat plateJournal of Fluid Mechanics, 27
Numerical solutions are presented for steady two‐dimensional symmetric flow past parabolic bodies in a uniform stream parallel to its axis. For this study, the full Navier‐Stokes equations and energy equation in parabolic coordinates were solved. A second order accurate finite difference scheme on a non‐uniform grid was used. The solution domain does not exclude the leading edge region as it is usually done with boundary layer flows. A wide range of Reynolds number ( R e ) is studied for different values of Prandtl number ( P r ). It is found that the average Nusselt number ( Nu ) increases as ( P r ) increases meanwhile, ( Nu ) decreases with the increase in ( R e ).
International Journal of Numerical Methods for Heat and Fluid Flow – Emerald Publishing
Published: Feb 1, 2000
Keywords: Forced convection; Laminar flow; Numerical solutions
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