An approximate method for the efficient calculation of stagnation streamline quantities in hypersonic flows about spheres or cylinders is suggested. Based on the local similarity of the flow field the two-dimensional Navier-Stokes equations are simplified to a one-dimensional approximation for the stagnation streamline. The dimensionally reduced equations are solved with an implicit finite-volume scheme. Comparisons with fully two-dimensional Euler and Navier-Stokes calculations for flows about spheres are presented, that include perfect gas flows in chemical non-equilibrium. Comparisons with a number of experiments conclude this report. (orig.)SIGLEAvailable from TIB Hannover: RN 8680(121) / FIZ - Fachinformationszzentrum Karlsruhe / TIB -...
A numerical code has been developed to solve the Viscous Shock Layer (VSL) equations for chemically ...
The stagnation-point heat flux on spheres in the High Enthalpy Shock Tunnel Göttingen (HEG) in the ...
The method described is an inverse one; the shock shape is chosen and the solution proceeds downstre...
The flow near the stagnation streamline of a blunt body is often attracted and analyzed by using the...
The numerical solution of a symmetric hypersonic blunt body flow in two space dimensions is consider...
AbstractThis study proposes a quasi-one-dimensional model to predict the chemical non-equilibrium fl...
A two-dimensional, axisymmetric, full Navier-Stokes solver has been developed with equilibrium and n...
The applicability of three numerical approximation methods of solving the Navier-Stokes equations (l...
This thesis investigates the nature of the development of two-dimensional laminar nonisothermal flow...
An analysis of nonequilibrium-dissociated stagnation point flow on highly cooled blunt bodies in a h...
The physical modeling of fluid flows neglecting effects due to diffusion, viscosity and heat conduct...
The solution of viscous shock-layer equations requires a stagnation point approach. Previous approac...
In this lecture we will (1) develop the governing PNS (Parobolized Navier-Stokes) equations for idea...
Results of solving the Navier-Stokes equations for chemically nonequilibrium, merged stagnation shoc...
A compensated compactness framework is established for sonic-subsonic approximate solutions to the t...
A numerical code has been developed to solve the Viscous Shock Layer (VSL) equations for chemically ...
The stagnation-point heat flux on spheres in the High Enthalpy Shock Tunnel Göttingen (HEG) in the ...
The method described is an inverse one; the shock shape is chosen and the solution proceeds downstre...
The flow near the stagnation streamline of a blunt body is often attracted and analyzed by using the...
The numerical solution of a symmetric hypersonic blunt body flow in two space dimensions is consider...
AbstractThis study proposes a quasi-one-dimensional model to predict the chemical non-equilibrium fl...
A two-dimensional, axisymmetric, full Navier-Stokes solver has been developed with equilibrium and n...
The applicability of three numerical approximation methods of solving the Navier-Stokes equations (l...
This thesis investigates the nature of the development of two-dimensional laminar nonisothermal flow...
An analysis of nonequilibrium-dissociated stagnation point flow on highly cooled blunt bodies in a h...
The physical modeling of fluid flows neglecting effects due to diffusion, viscosity and heat conduct...
The solution of viscous shock-layer equations requires a stagnation point approach. Previous approac...
In this lecture we will (1) develop the governing PNS (Parobolized Navier-Stokes) equations for idea...
Results of solving the Navier-Stokes equations for chemically nonequilibrium, merged stagnation shoc...
A compensated compactness framework is established for sonic-subsonic approximate solutions to the t...
A numerical code has been developed to solve the Viscous Shock Layer (VSL) equations for chemically ...
The stagnation-point heat flux on spheres in the High Enthalpy Shock Tunnel Göttingen (HEG) in the ...
The method described is an inverse one; the shock shape is chosen and the solution proceeds downstre...