๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

A Finite-Difference Scheme for Three-Dimensional Incompressible Flows in Cylindrical Coordinates

โœ Scribed by R. Verzicco; P. Orlandi


Publisher
Elsevier Science
Year
1996
Tongue
English
Weight
508 KB
Volume
123
Category
Article
ISSN
0021-9991

No coin nor oath required. For personal study only.

โœฆ Synopsis


A finite-difference scheme for the direct simulation of the incompressible time-dependent three-dimensional Navier-Stokes equa- [6] proposed an accurate method for three-dimensional tions in cylindrical coordinates is presented. The equations in primipipe flows with Jacobi polynomials for the radial direction. tive variables (v r , v , v z and p) are solved by a fractional-step method These polynomials were introduced to minimize the together with an approximate-factorization technique. Cylindrical coupling of the momentum equations, nevertheless the coordinates are singular at the axis; the introduction of the radial discretization produced large nondiagonal sparse matrices flux q r ฯญ r ะธ v r on a staggered grid simplifies the treatment of the region at r ฯญ 0. The method is tested by comparing the evolution to be inverted. Buell et al. [7] developed a Galerkin of a free vortex ring and its collision with a wall with the theory, method to simulate the natural convection in a circular experiments, and other numerical results. The formation of a tripolar enclosure. In the radial direction Bessel functions were vortex, where the highest vorticity is at r ฯญ 0, is also considered.

used and the condition of finiteness of the solution was

Finally to emphasize the accurate treatment near the axis, the motion of a Lamb dipole crossing the origin is simulated. แฎŠ 1996 Aca-applied at r ฯญ 0. However, the Galerkin method was demic Press, Inc.

used to reduce the linearized perturbation equations to an eigenvalue problem and no information was provided about the extension of the method to the full Navier-


๐Ÿ“œ SIMILAR VOLUMES


A Finite-Dimensional Attractor for Three
โœ Josef Mรกlek; Jindล™ich Neฤas ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 827 KB

The asymptotic behavior of the flow for a system of the Navier Stokes type is investigated. In the considered model, the viscous part of the stress tensor is generally a nonlinear function of the symmetric part of the velocity gradient. Provided that the function describing this dependence satisfies

Finite Difference Schemes for Incompress
โœ Weinan E; Jian-Guo Liu ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 434 KB

together with perspectives on the application of real space renormalization procedures to vortex methods based on We consider finite difference schemes based on the impulse density variable. We show that the original velocity-impulse density the impulse density. formulation of Oseledets is margina

A Fully Conservative Second-Order Finite
โœ F.E. Ham; F.S. Lien; A.B. Strong ๐Ÿ“‚ Article ๐Ÿ“… 2002 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 150 KB

A second-order-accurate finite difference discretization of the incompressible Navier-Stokes is presented that discretely conserves mass, momentum, and kinetic energy (in the inviscid limit) in space and time. The method is thus completely free of numerical dissipation and potentially well suited to

A convergent three-level finite differen
โœ Weizhong Dai; Lixin Shen; Raja Nassar ๐Ÿ“‚ Article ๐Ÿ“… 2003 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 126 KB

## Abstract Heat transport at the microscale is of vital importance in microtechnology applications. The heat transport equation is different from the traditional heat diffusion equation since a secondโ€order derivative of temperature with respect to time and a thirdโ€order mixed derivative of temper