dc.contributor | Strathclyde University | |
dc.contributor | Universidade Estadual Paulista (Unesp) | |
dc.date.accessioned | 2014-05-27T11:18:17Z | |
dc.date.accessioned | 2022-10-05T17:34:53Z | |
dc.date.available | 2014-05-27T11:18:17Z | |
dc.date.available | 2022-10-05T17:34:53Z | |
dc.date.created | 2014-05-27T11:18:17Z | |
dc.date.issued | 1997-11-30 | |
dc.identifier | International Journal for Numerical Methods in Fluids, v. 25, n. 10, p. 1119-1135, 1997. | |
dc.identifier | 0271-2091 | |
dc.identifier | http://hdl.handle.net/11449/65232 | |
dc.identifier | 10.1002/(SICI)1097-0363(19971130)25:10<1119::AID-FLD610>3.0.CO;2-4 | |
dc.identifier | 2-s2.0-0031277562 | |
dc.identifier | 8232289412108723 | |
dc.identifier | 0000-0002-2080-8053 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/3915181 | |
dc.description.abstract | A fourth-order numerical method for solving the Navier-Stokes equations in streamfunction/vorticity formulation on a two-dimensional non-uniform orthogonal grid has been tested on the fluid flow in a constricted symmetric channel. The family of grids is generated algebraically using a conformal transformation followed by a non-uniform stretching of the mesh cells in which the shape of the channel boundary can vary from a smooth constriction to one which one possesses a very sharp but smooth corner. The generality of the grids allows the use of long channels upstream and downstream as well as having a refined grid near the sharp corner. Derivatives in the governing equations are replaced by fourth-order central differences and the vorticity is eliminated, either before or after the discretization, to form a wide difference molecule for the streamfunction. Extra boundary conditions, necessary for wide-molecule methods, are supplied by a procedure proposed by Henshaw et al. The ensuing set of non-linear equations is solved using Newton iteration. Results have been obtained for Reynolds numbers up to 250 for three constrictions, the first being smooth, the second having a moderately sharp corner and the third with a very sharp corner. Estimates of the error incurred show that the results are very accurate and substantially better than those of the corresponding second-order method. The observed order of the method has been shown to be close to four, demonstrating that the method is genuinely fourth-order. © 1977 John Wiley & Sons, Ltd. | |
dc.language | eng | |
dc.relation | International Journal for Numerical Methods in Fluids | |
dc.relation | 1.673 | |
dc.relation | 1,183 | |
dc.rights | Acesso restrito | |
dc.source | Scopus | |
dc.subject | Fourth-order methods | |
dc.subject | Navier-Stokes equations | |
dc.subject | Boundary conditions | |
dc.subject | Channel flow | |
dc.subject | Error analysis | |
dc.subject | Iterative methods | |
dc.subject | Navier Stokes equations | |
dc.subject | Nonlinear equations | |
dc.subject | Problem solving | |
dc.subject | Reynolds number | |
dc.subject | Vortex flow | |
dc.subject | Fourth order method | |
dc.subject | Newton iteration | |
dc.subject | Computational fluid dynamics | |
dc.subject | channel | |
dc.subject | fluid flow | |
dc.subject | vorticity | |
dc.subject | channel flow | |
dc.subject | fourth-order methods | |
dc.title | Fourth-order method for solving the Navier-Stokes equations in a constricting channel | |
dc.type | Artigo | |