Comparative criteria for finite-difference formulations for problems of fluid flow
β Scribed by Akshai K. Runchal
- Publisher
- John Wiley and Sons
- Year
- 1977
- Tongue
- English
- Weight
- 624 KB
- Volume
- 11
- Category
- Article
- ISSN
- 0029-5981
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
This paper concerns a technique for providing quantitative and qualitative answers to the questions related to accuracy and stability of finiteβdifference schemes. It is applicable to both the unsteady and the steady flows. The application of the technique provides comparative information about the amplitudes and the speeds of propagation of the numerical and analytic solutions. The difference between the two solutions is characterized in terms of a βfalseβ propagation speed and βfalseβ diffusion parameters for the numerical schemes.
The technique is applied to a number of commonly used finiteβdifference schemes and it is concluded that the use of central differences for the convective terms and/or explicit formulations tends to increase the amplitudes and wave speeds. The opposite effects on the amplitudes and wave speeds are produced by upwind or βdonorβ cell differences and/or implicit formulations.
π SIMILAR VOLUMES
In this work we discuss stable equal-order finite element formulations for incompressible flow problems based on Petrov-Galerkin methods, constructed by adding to the classical Galerkin formulation leastsquares of the governing equations. Continuous and discontinuous pressure interpolations are cons
boundary. Recently, this result was improved in [15] to show second-order convergence of solutions including Thom's vorticity condition for solving the incompressible Navier-Stokes equations is generally known as a first-order method since boundary vorticity for the steady Stokes equations using the
A finite element formulation for the steady laminar flow of an incompressible fluid with microstructure has been developed. The particular fluids considered are commonly known as micropolar fluids, in which case suspended particulate microstructures are modelled by an 'extended' continuum formulatio