• Refine Query
  • Source
  • Publication year
  • to
  • Language
  • 2
  • 1
  • Tagged with
  • 3
  • 3
  • 3
  • 3
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • 2
  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
1

Simulação numérica de escoamentos de fluidos utilizando diferenças finitas generalizadas / Numerical simulation of fluid flow using generalized finite differences

Santos, Fernanda Olegario dos 24 November 2005 (has links)
Este trabalho apresenta parte de um sistema de simulação integrado para escoamento de fluido incompressível bidimensional em malhas não estruturadas denominado UmFlow-2D. O sistema consiste de três módulos: um módulo modelador, um módulo simulador e um módulo visualizador. A parte do sistema apresentado neste trabalho é o módulo simulador. Este módulo, implementa as equações de Navier-Stokes. As equações governantes são discretizadas pelo método de diferenças finitas generalizadas e os termos convectivos pelo método semi-lagrangeano. Um método de projeção é empregado para desacoplar as componentes da velocidade e pressão. O gerenciamento da malha, não estruturada é feito pela estrutura de dados SHE. Os resultados numéricos obtidos pelo UmFlow-2D são comparados com soluções analíticas e soluções numéricas de outros trabalhos. / This work presents an integratc simulation system, called UmFlow-2D, wich aims a,t simulating two-dimensional íncompressible fluid flow using unstructed mesh. The system is divided three modules: modeling module, simulation module and visualization module. In this work we present the simulation module. The simulation module implements the Navier-Stokes equation. The governing equations are discretized by a generalized flnite dillerence method and the convective terms by semi-lagrangean method. A projection method is employed to uncouple the velocity componentes and pressure. The management at the unstructed mesh is ready using a data structure called SHE. The numérica! results are compared with analytical solutions and numerical simulations of other works.
2

Generalized Finite Difference Method In Elastodynamics Using Perfectly Matched Layer

Korkut, Fuat 01 July 2012 (has links) (PDF)
This study deals with the use of the generalized finite difference method (GFDM) in perfectly matched layer (PML) analysis of the problems in wave mechanics, in particular, in elastodynamics. It is known that PML plays the role of an absorbing layer, for an unbounded domain, eliminating reflections of waves for all directions of incidence and frequencies. The study is initiated for purpose of detecting any possible advantages of using GFDM in PML analysis: GFDM is a meshless method suitable for any geometry of the domain, handling the boundary conditions properly and having an easy implementation for PML analysis. In the study, first, a bounded 2D fictitious plane strain problem is solved by GFDM to determine its appropriate parameters (weighting function, radius of influence, etc.). Then, a 1D semi-infinite rod on elastic foundation is considered to estimate PML parameters for GFDM. Finally, the proposed procedure, that is, the use of GFDM in PML analysis, is assessed by considering the compliance functions (in frequency domain) of surface and embedded rigid strip foundations. The surface foundation is assumed to be supported by three types of soil medium: rigid strip foundation on half space (HS), on soil layer overlying rigid bedrock, and on soil layer overlying HS. For the embedded rigid strip foundation, the supporting soil medium is taken as HS. In addition of frequency space analyses stated above, the direct time domain analysis is also performed for the reaction forces of rigid strip foundation over HS. The results of GFDM for both frequency and time spaces are compared with those of finite element method (FEM) with PML and boundary element method (BEM), when possible, also with those of other studies. The excellent matches observed in the results show the reliability of the proposed procedure in PML analysis (that is, of using GFDM in PML analysis).
3

Simulação numérica de escoamentos de fluidos utilizando diferenças finitas generalizadas / Numerical simulation of fluid flow using generalized finite differences

Fernanda Olegario dos Santos 24 November 2005 (has links)
Este trabalho apresenta parte de um sistema de simulação integrado para escoamento de fluido incompressível bidimensional em malhas não estruturadas denominado UmFlow-2D. O sistema consiste de três módulos: um módulo modelador, um módulo simulador e um módulo visualizador. A parte do sistema apresentado neste trabalho é o módulo simulador. Este módulo, implementa as equações de Navier-Stokes. As equações governantes são discretizadas pelo método de diferenças finitas generalizadas e os termos convectivos pelo método semi-lagrangeano. Um método de projeção é empregado para desacoplar as componentes da velocidade e pressão. O gerenciamento da malha, não estruturada é feito pela estrutura de dados SHE. Os resultados numéricos obtidos pelo UmFlow-2D são comparados com soluções analíticas e soluções numéricas de outros trabalhos. / This work presents an integratc simulation system, called UmFlow-2D, wich aims a,t simulating two-dimensional íncompressible fluid flow using unstructed mesh. The system is divided three modules: modeling module, simulation module and visualization module. In this work we present the simulation module. The simulation module implements the Navier-Stokes equation. The governing equations are discretized by a generalized flnite dillerence method and the convective terms by semi-lagrangean method. A projection method is employed to uncouple the velocity componentes and pressure. The management at the unstructed mesh is ready using a data structure called SHE. The numérica! results are compared with analytical solutions and numerical simulations of other works.

Page generated in 0.1341 seconds