Two Different Formulations for Solving the Navier- Stokes Equations with Moderate and High Reynolds Numbers

In this work, we discuss the numerical solution of the Taylor vortex and the lid-driven cavity problems. Both problems are solved using the Stream function-vorticity formula- tion of the Navier-Stokes equations in 2D. Results are obtained using a fixed point iterative method and working with matrixe...

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Autores:
Tipo de recurso:
Book
Fecha de publicación:
2021
Institución:
Universidad de Bogotá Jorge Tadeo Lozano
Repositorio:
Expeditio: repositorio UTadeo
Idioma:
eng
OAI Identifier:
oai:expeditiorepositorio.utadeo.edu.co:20.500.12010/16715
Acceso en línea:
https://www.intechopen.com/books/computational-fluid-dynamics-basic-instruments-and-applications-in-science/two-different-formulations-for-solving-the-navier-stokes-equations-with-moderate-and-high-reynolds-n
http://hdl.handle.net/20.500.12010/16715
Palabra clave:
Ecuaciones de Navier - Stokes
Formulación de velocidad vorticidad
Número de Reynolds
Formulación de función de flujo vorticidad
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Abierto (Texto Completo)
Description
Summary:In this work, we discuss the numerical solution of the Taylor vortex and the lid-driven cavity problems. Both problems are solved using the Stream function-vorticity formula- tion of the Navier-Stokes equations in 2D. Results are obtained using a fixed point iterative method and working with matrixes A and B resulting from the discretization of the Laplacian and the advective term, respectively. We solved both problems with Reynolds numbers in the range of 3200 ≤ Re ≤ 7500. Results are also obtained using the velocity-vorticity formulation of the Navier-Stokes equations. In this case, we are using only the fixed point iterative method. We present results for the lid-driven cavity prob- lem and for the Stream function-vorticity formulation with Reynolds numbers in the range of 3200 ≤ Re ≤ 7500. As the Reynolds number increases, the time and the space step size have to be refined. We show results for 3200 ≤ Re ≤ 20,000. The numerical scheme with the velocity-vorticity formulation uses a smaller step size for both time and space. Results are not as good as with the Stream function-vorticity formulation, although the way the scheme behaves gives us another point of view on the behavior of fluids under different numerical schemes and different formulation.