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MESTRADO EM CONSTRUÇÃO METÁLICA
DEPARTAMENTO DE ENGENHARIA CIVIL
ESCOLA DE
UNIVERSIDADE FEDERAL DE OURO PRETO
ALEXANDRE DA SILVA GALVÂO
DISSERTAÇÃO DE MESTRADO
Orientadores: Ricardo Azoubel da Mota Silveira
Convênio USIMINAS/UFOP/FUNDAÇÃO Ouro Preto, março de 2000
Formulações Não-Lineares de Elementos Finitos para Análise
UNIVERSIDADE FEDERAL DE OURO PRETO - ESCOLA DE MINASDEPARTAMENTO DE ENGENHARIA CIVIL
PROGRAMA DE PÓS – GRADUAÇÃO EM ENGENHARIA CIVIL
Formulações Não-Lineares de Elementos Finitos para Análisede Sistemas Estruturais Metálicos Reticulados Planos
AUTOR: ALEXANDRE DA SILVA GALVÃO
ORIENTADOR: Prof. Dr. Ricardo Azoubel da Mota Silveira
Dissertação apresentada ao Programa de Pós-Graduação do Departamento de EngenhariaCivil da Escola de Minas da UniversidadeFederal de Ouro Preto, como parte integrantedos requisitos para obtenção do título deMestre em Engenharia Civil, área deconcentração: Construções Metálicas.
Ouro Preto, março de 2000.
III
“...A ciência é a potência do homem, e, o amor, a sua força;o homem só se torna homem pela inteligência, mas só é homempelo coração.
Saber, amar e poder; eis a vida completa.”
Henri-Frédéric Amiel (1821-1891)
A minha família.
IV
MEUS AGRADECIMENTOS
“Dê-me uma alavanca e um ponto de apoio,e eu faço mover o mundo.”
Arquimedes (287AC-217AC)
• Aos meus pais e ao meu irmão, por serem o meu mundo.
• Ao meu professor e orientador Ricardo Azoubel da Mota Silveira, por ter
sido a alavanca e o apoio dessa nossa empreitada.
• À Escola de Minas, por ser parte da minha vida.
• Aos meus colegas, pelo prazer da convivência nesses dois anos.
• À CAPES e à USIMINAS, pela ajuda financeira.
V
RESUMO
Este trabalho tem como principais objetivos o estudo e a implementação computacional
de formulações geometricamente não-lineares para elementos finitos reticulados planos
encontradas na literatura recente. Essas formulações, além de permitir a determinação da matriz
de rigidez e do vetor de forças internas de forma direta, podem ser acopladas com relativa
facilidade a várias estratégias de solução não-linear.
Procurando fornecer diferentes opções de modelagem de problemas de instabilidade
usando esses elementos finitos reticulados planos, foram implementadas as seguintes
formulações geometricamente não-lineares: (i) formulações definidas por Alves (1993b) e
Torkamani et al. (1997), implementadas aqui com procedimentos distintos de se avaliar o vetor
de forças internas: forma total e forma incremental; (ii) formulações propostas por Yang e Kuo
(1994), que se basearam em modelos linearizado, linearizado-simplificado e com termos de
ordem elevada; foram ainda introduzidas por esses autores duas abordagens diferentes,
implementadas neste trabalho, de obtenção do vetor de forças internas: deslocamentos naturais
incrementais e rigidez externa; e (iii) formulações em referencial Lagrangiano total, propostas
por Pacoste e Eriksson (1997), baseadas em diferentes relações cinemáticas e definições de
deformações; cinco formulações foram sugeridas por esses pesquisadores, onde todas foram
testadas no presente trabalho.
Essas formulações foram adaptadas à metodologia de solução não-linear que usa o
método de Newton-Raphson (Silveira, 1995), acoplado às diferentes estratégias de incremento
de carga e de iteração que permitem a ultrapassagem de pontos críticos (bifurcação e limite) que
possam existir ao longo da trajetória de equilíbrio.
A avaliação da eficiência computacional dessas formulações é feita no final do trabalho
através da análise de problemas estruturais fortemente não-lineares encontrados na literatura.
• Alves, R.V. (1993b). Formulação para Análise Não-Linear Geométrica em Referencial LagrangianoAtualizado. 3o Seminário de Doutorado, COPPE/UFRJ.• Pacoste, C. e Eriksson, A. (1997). Beam elements in instability problems. Comput. Methods Appl.Mech. Engrg., No 144, p. 163-197.• Silveira, R.A.M. (1995). Análise de Elementos Estruturais Esbeltos com Restrições Unilaterais deContato. Tese de Doutorado. PUC-RJ, Rio de Janeiro, RJ.• Torkamani, M.A.M., Sonmez, M. e Cao, J. (1997). Second-Order Elastic Plane-Frame Analysis UsingFinite-Element Method. Journal of Structural Engineering, Vol 12, No 9, p. 1225-1235.• Yang, Y.B. e Kuo, S.B. (1994). Theory & Analysis of Nonlinear Framed Structures, Prentice Hall.
VI
ABSTRACT
The main objectives of this work are the computational implementation and study of
geometrically non-linear formulations for two dimensional frame elements. In the formulations
here studied, the stiffness matrix and the internal forces vector can be obtained directly, and
they can be easily coupled to different non-linear solution strategies.
In order to give different options for the solutions of instability problems these two
dimensional frame elements, the following geometrically non-linear formulations were
implemented: (i) Alves (1993b) e Torkamani et al. (1997) formulations, where two different
procedures to obtain the internal forces vector (total and incremental approaches) were tested;
(ii) Yang and Kuo (1994) formulations, where a simplified, a linear-simplified and a higher
order planar frame element were used; these authors introduced two methodologies to obtain the
internal load vector: natural deformation and external stiffness approaches; (iii) Pacoste and
Eriksson (1997) formulations, where a total reference frame (total Lagrangian formulation) was
adopted, and different kinematic assumptions and strain definitions were used; five different
formulations were presented and tested in the present work.
These formulations were coupled to the non-linear solution methodology implemented
initially by Silveira (1995), which solves the resulting non-linear equations and obtains the non-
linear equilibrium paths through the Newton-Raphson method together with path following
techniques, such as the arc-length schemes proposed by Crisfield and orthogonal residual
procedures derived by Krenk.
The performance and capacity of these formulations are illustrated by means of several
numerical examples.
• Alves, R.V. (1993b). Formulação para Análise Não-Linear Geométrica em Referencial LagrangianoAtualizado. 3o Seminário de Doutorado, COPPE/UFRJ.• Pacoste, C. and Eriksson, A. (1997). Beam elements in instability problems. Comput. Methods Appl.Mech. Engrg., No 144, p. 163-197.• Silveira, R.A.M. (1995). Análise de Elementos Estruturais Esbeltos com Restrições Unilaterais deContato. Tese de Doutorado. PUC-RJ, Rio de Janeiro, RJ.• Torkamani, M.A.M., Sonmez, M. and Cao, J. (1997). Second-Order Elastic Plane-Frame AnalysisUsing Finite-Element Method. Journal of Structural Engineering, Vol 12, No 9, p. 1225-1235.• Yang, Y.B. and Kuo, S.B. (1994). Theory & Analysis of Nonlinear Framed Structures, Prentice Hall.
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SUMÁRIO
Resumo#$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$!
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Lista de Figuras$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$ %"
Lista de Tabelas $$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$%"!
Lista de Símbolos $$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$%!"
Capítulo 1#INTRODUÇÃO
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Capítulo 3 – FORMULAÇÕES NÃO-LINEARES DE ELEMENTOS FINITOS:ALVES (1993b) e TORKAMANI et al. (1997)
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Capítulo 4 – FORMULAÇÕES NÃO-LINEARES DE ELEMENTOS FINITOS:YANG e KUO(1994)
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Capítulo 5 – FORMULAÇÕES NÃO-LINEARES DE ELEMENTOS FINITOS:PACOSTE e ERIKSSON (1997)
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E$:$:#/HGL#(OHGZUQH#4OHHLKZUQML$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$'BE
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Capítulo 8#CONCLUSÕES E SUGESTÕES
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LISTA DE FIGURAS
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Capítulo 2
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LISTA DE TABELAS
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Capítulo 7
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6QbIUQ#E$BQ#(QH[Q#GHVKOGQi#!QULHIR#MI#SGH#83s#-" $$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$'''
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6QbIUQ#E$'Ab!QULH#MI#Sh.3s-"#FL#3L#NLFKL#MI#bO^ZHGQWXL $$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$'3=
6QbIUQ#E$''!QULHIR#MQ#GQ[Q#MI#bO^ZHGQWXL#JmfOJQi#SQGLRKI#I#-HOjRRLF#_'??Ec$$$':=
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LISTA DE SÍMBOLOS
Capítulo 2
λ SQHTJIKHL#MI#GQH[Q#HIRNLFRm`IU#NIUL#IRGQULFQJIFKL#MI#Fr$
ζ 6LUIHTFGOQ#QL#HIRVMZL#HInZIHOMQ#FL#NHLGIRRL#MI#GLF`IH[rFGOQ$
ζ'
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K yUKOJQ#GLF^O[ZHQWXL#MI#InZOUVbHOL#NHLGIRRQMQ$
K#z#∆K (LF^O[ZHQWXL#MI#InZOUVbHOL#NHLGZHQMQ#FL#NQRRL#MI#GQH[Q#GLHHIFKI$
u !IKLH#MI#MIRULGQJIFKLR#FLMQOR$
∆u !IKLH#MI#MIRULGQJIFKLR#FLMQOR#OFGHIJIFKQOR$
∆u_j@'c#I#∆u#j !IKLH# MI# MIRULGQJIFKLR# FLMQOR# OFGHIJIFKQOR# Q`QUOQML# FQ# OKIHQWXL
QFKIHOLH#_j@'c#I#FQ#OKIHQWXL#GLHHIFKI#j$
∆uA "FGHIJIFKL#OFOGOQU#MLR#MIRULGQJIFKLR#FLMQOR$
δu !IKLH#MI#MIRULGQJIFKLR#HIROMZQOR$
δug SQHGIUQ#MI#δu HI^IHIFKI#{R#^LHWQR#HIROMZQOR#g$
δu_j@'c#I#δuj !IKLH# MI# MIRULGQJIFKLR# HIROMZQOR# OFGHIJIFKQOR# Q`QUOQML# FQ# OKIHQWXL
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δur SQHGIUQ#MI#δu HI^IHIFKI#{R#^LHWQR#MI#HI^IHrFGOQ#Fr$
δu6 !IKLH#MLR#MIRULGQJIFKLR#KQF[IFGOQOR$
jwuδ !IKLH#MLR#MIRULGQJIFKLR#OKIHQKO`LR$
Capítulo 3
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ψ .LKQWXL#MI#GLHNL#HV[OML#_KLKQU#LZ#OFGHIJIFKQUc$
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∆Π# "FGHIJIFKL#MQ#IFIH[OQ#NLKIFGOQU#KLKQU$
∆σ# "FGHIJIFKL#MI#KIFRXL#QfOQU$
∆εff "FGHIJIFKL#MI#MI^LHJQWXL#QfOQU$
∆Iff SQHGIUQ#UOFIQH#MI#∆εff$
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∆un !IKLH#MI#MIRULGQJIFKLR#FQKZHQOR#OFGHIJIFKQOR$
Z∆ "FGHIJIFKL# MI# MIRULGQJIFKL# QfOQU# MI# ZJ# NLFKL# MORKQFKI# }# MQ# UOFhQ
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∆># "FGHIJIFKL#MQ#IFIH[OQ#OFKIHFQ#MI#MI^LHJQWXL$
∆!# "FGHIJIFKL#MQ#IFIH[OQ#NLKIFGOQU#MQR#^LHWQR#IfKIHFQR$
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O desenvolvimento de novos materiais e técnicas construtivas, bem como os
recursos computacionais disponíveis hoje, têm levado ao emprego de elementos
estruturais cada vez mais esbeltos. A medida que se aumenta a esbeltez de um dado
elemento estrutural, este torna-se cada vez mais susceptível a sofrer grandes deflexões
laterais, que tendem a ocorrer antes da ruptura física. Para se projetar esse tipo de
estrutura deve-se usar o chamado critério de estabilidade. O estudo da não-linearidade
geométrica desses elementos estruturais torna-se, portanto, cada vez mais importante,
possibilitando em certos casos o aparecimento de múltiplas configurações de equilíbrio
(estáveis e instáveis), e a existência de pontos críticos (pontos limites e pontos de
bifurcação) ao longo do caminho não-linear de equilíbrio onde a estrutura pode exibir
saltos dinâmicos.
Portanto, o conhecimento do comportamento não-linear de elementos estruturais
esbeltos, tais como colunas, arcos, anéis, placas e cascas, é de fundamental importância
na solução de problemas de estabilidade/instabilidade local e/ou global de sistemas
estruturais complexos, pois na maioria das aplicações de engenharia esses sistemas são
formadas a partir da união desses elementos.
A análise da estabilidade de sistemas estruturais esbeltos através do Método dos
Elementos Finitos (MEF) envolve invariavelmente a solução de um sistema de equações
algébricas não-lineares. Como relatado no artigo de Riks (1979) e também destacado
em Silveira (1995), existem basicamente duas classes de solução desse sistema de
equações:
2
1. Adaptação computacional do método de perturbação desenvolvido por Koiter
(1970). Durante muitos anos o método de Koiter foi considerado inadequado ao
contexto de elementos finitos, entretanto, trabalhos recentes como os
desenvolvidos por Salerno e Lanzo (1997) e Wu e Wang (1997) provam o
contrário, renovando o interesse dos pesquisadores por esse método;
2. Métodos que procuram resolver as equações não-lineares passo a passo. Incluídos
nessa segunda classe estão os métodos puramente incrementais, as técnicas
baseadas em relações de rigidez secante e os esquemas que combinam
procedimentos incrementais e iterativos, que são atualmente considerados os mais
eficientes e que serão utilizado no presente trabalho.
Recentemente, muitos pesquisadores têm desenvolvido formulações
geometricamente não-lineares para elementos finitos (Alves 1993a-b; Crisfield, 1991;
Yang e Kuo, 1994; Pacoste e Eriksson, 1997; Torkamani et al., 1997; Neuenhofen e
Fillippou, 1997 e 1998), que têm sido adequadamente empregadas na modelagem de
vários sistemas estruturais esbeltos. Essas formulações permitem a determinação da
matriz de rigidez e do vetor de forças internas de forma direta e podem ser acopladas
com relativa facilidade às várias estratégias de solução não-linear.
Essas considerações motivaram a adoção desse tema para a presente dissertação
de mestrado.
3
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O presente trabalho é parte integrante das seguintes linhas de pesquisa do
Mestrado em Construção Metálica (Deciv/EM/UFOP):
• Análise Numérica e Computacional em Engenharia: tem como objetivo a
aplicação de métodos numéricos, como o método dos elementos finitos (MEF) e/ou o
método dos elementos de contorno (MEC), na determinação de respostas de sistemas de
engenharia;
• Instabilidade das Estruturas: objetiva o estudo do equilíbrio e estabilidade de
elementos estruturais esbeltos (colunas, arcos, anéis, placas e cascas) submetidos a
carregamentos diversos.
O principal objetivo deste trabalho é o estudo e implementação computacional de
formulações geometricamente não-lineares, para elementos finitos reticulados planos.
Essas formulações serão integradas à metodologia de solução numérica implementada
por Silveira (1995) e expandida por Rocha (2000), que implementou com sucesso
algumas estratégias de solução não-linear encontradas recentemente na literatura.
A seguir, na Seção (1.3), é feita uma revisão bibliográfica onde atenção especial é
dada aos trabalhos que tratam diretamente de formulações geometricamente não-
lineares.
No Capítulo 2 é feita uma explanação geral sobre a metodologia de solução não-
linear adotada, apresentando de maneira resumida as estratégias de incremento de carga
e iterações usadas no presente trabalho.
Os Capítulos 3, 4 e 5 pretendem apresentar de forma detalhada o desenvolvimento
teórico das formulações de elementos finitos não-lineares, que é o principal objeto de
estudo desta dissertação. Na descrição dessas formulações merecem destaque as
relações deformação-deslocamento, as deduções das equações de equilíbrio, o tipo de
elemento finito e as funções de interpolação utilizadas e, finalmente, a obtenção dos
vetores de forças internas e das matrizes de rigidez.
O Capítulo 6 apresenta de forma resumida os procedimentos adotados na
implementação computacional das formulações apresentadas nos Capítulos 3, 4 e 5,
onde atenção especial é dada à montagem da matriz de rigidez e do vetor de forças
internas.
4
As formulações apresentadas nos Capítulos 3, 4 e 5 são analisadas no Capítulo 7,
que apresenta exemplos de problemas estruturais encontrados na literatura. A Seção
(7.2) fornece cinco exemplos clássicos que, por serem mais simples, têm soluções
analíticas (exatas) encontradas na literatura. Em função da confiabilidade dessas
análises, seus resultados têm o objetivo de avaliar a qualidade dos resultados produzidos
pelas diferentes formulações. Com o intuito de validar as observações feitas na Seção
(7.2), são abordados na Seção (7.3) cinco problemas estruturais de estabilidade elástica
fortemente não-lineares, cujas soluções, obtidas numericamente por diversos
pesquisadores, são encontradas na literatura.
Finalmente, no Capítulo 8, são apresentadas as conclusões sobre o emprego das
diversas formulações analisadas nos exemplos do Capítulo 7. São fornecidas também
algumas sugestões para o desenvolvimento de trabalhos futuros.
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5
comparativo entre as formulações de Argyris (1964), Martin (1965), Jennings (1968),
Mallet e Marçal (1968) e Powell (1969).
Epstein e Murray (1976) desenvolveram uma formulação para elementos de
pórticos planos análoga à formulação para elementos de casca, para grandes
deformações, apresentada por Budiansky (1968).
Recentemente, formulações em referenciais Lagrangianos (RLT e RLA) foram
apresentadas por vários pesquisadores, dos quais pode-se citar: Wen et al. (1983);
Chajes et al. (1987); Goto et al. (1987); Wong e Loi (1990); Alves (1993a-b) e
Torkamani et al. (1997). Yang e Kuo (1994) sugeriram uma forma incremental de se
calcular o vetor de forças internas com duas abordagens diferentes para os
deslocamentos nodais: deslocamentos naturais incrementais e rigidez externa. Pacoste e
Eriksson (1995 e 1997) introduziram formulações em RLT baseadas em relações
deformação-deslocamento denominadas ‘relações melhoradas’, com a não-linearidade
expressa por funções trigonométricas.
Singh e Singh (1992) propuseram um modelo com matriz de rigidez e vetor de
forças internas modificáveis de acordo com a natureza das forças axiais.
Um procedimento geral para a obtenção de matrizes de rigidez simétricas foi
proposto por Moran et al. (1998). Neuenhofer e Filippou (1998) propuseram uma
formulação baseada no método da flexibilidade.
Crisfield (1991) afirmou em seu livro que o termo corrotacional tem sido
utilizado na literatura em diferentes contextos, sendo portanto, como afirmam ainda
Pacoste e Eriksson (1997), uma denominação inconsistente. A idéia central desse tipo
de formulação é o cálculo da matriz rigidez e do vetor de forças internas no campo dos
deslocamentos naturais (ou locais), que são os deslocamentos referidos a um sistema de
coordenadas que é atualizado a cada passo de carga, acompanhando a rotação sofrida
pelo elemento. Das formulações com abordagem corrotacional publicadas recentemente
pode-se destacar a formulação em RLA proposta por Crisfield (1991) e as formulações
desenvolvidas em RLT por Pacoste e Eriksson (1997) e Xu e Mirmiran (1997).
Ao contrário da teoria de vigas de Bernoulli, na teoria de vigas de Timoshenko os
efeitos devidos às deformações cisalhantes na seção transversal não são desprezados no
cálculo da rigidez da estrutura. Formulações baseadas na teoria de vigas de Timoshenko
6
foram propostas por Iwakuma (1990), Lee et al. (1994), Petrolito (1995) e Pacoste e
Eriksson (1997).
Os sistemas estruturais formados por barras curvas podem ser analisados com as
formulações de elementos finitos de vigas retas. Porém, com o intuito de melhorar a
eficiência dessas análises foram desenvolvidas formulações de elementos finitos curvos.
Entre os trabalhos recentes, merecem destaque as formulações de elementos curvos
propostas por Marquist e Wang (1989), Kim e Kim (1998), e Raveendranath et al.
(1999); e as formulações de elementos parabólicos propostas por Litewka e Rakowski
(1997 e 1998).
Paralelamente aos elementos para análises bidimensionais, têm-se desenvolvido o
estudo de elementos finitos para análise geometricamente não-linear de pórticos
tridimensionais. Sabe-se de antemão que uma formulação não-linear tridimensional não
é uma simples extensão de uma formulação bidimensional porque as rotações finitas
tridimensionais não são quantidades vetoriais. Recentemente, vários pesquisadores têm
publicado formulações não-lineares para análise estática de pórticos tridimensionais.
Entre eles pode-se destacar Yang e Kuo (1994), que propôs formulações para elementos
tridimensionais retos e curvos; Choi e Lim (1995), com uma formulação de elemento
curvo; al.et coviIbrahimbeg ′ (1996); Ammar et al. (1996), com formulações para
elementos de vigas esbeltas e não-esbeltas; Matsununga (1996), com uma formulação
para pilares não-esbeltos; Pacoste e Eriksson (1997), que propuseram formulações com
abordagem total e corrotacional; Rhim e Lee (1998), que desenvolveram uma
formulação dando um tratamento vetorial à geometria do problema; e Li (1998), que
elaborou uma formulação aplicando a teoria de rotações finitas.
Tem-se produzido também um grande número de formulações geometricamente
não-lineares incluindo análise elasto-plástica de sistemas estruturais reticulados. Essas
formulações têm como principal característica a adotação do critério de escoamento
plástico na determinação das tensões. Nessa linha de pesquisa pode-se destacar os
seguintes trabalhos já publicados: Hsiao et al. (1988), Lee (1988), Meek e Loganathan
(1990), Chang-New Chen (1996), Park e Lee (1996), Ovunc e Ren (1996), Saje et al.
(1997), Saje et al. (1998), Waszczyszyn e Michalska (1998).
7
Nos últimos 20 anos, os avanços tecnológicos e as exigências do mercado de
engenharia, que introduziram maior complexidade e eficiência aos cálculos estruturais,
levaram os pesquisadores a procurarem metodologias de solução que ao mesmo tempo
produzissem resultados precisos e fossem de rápido processamento. Juntamente com as
pesquisas relativas ao desenvolvimento de formulações não-lineares, muitos trabalhos
têm sido produzidos com a finalidade de se determinar a melhor estratégia de solução
não-linear. Os métodos que têm mostrado maior eficiência são os que combinam
procedimentos incrementais e iterativos. Como trabalhos pioneiros podem ser citados os
desenvolvidos por: Argyris (1964), com a aplicação de um método incremental para
solução não-linear; Mallet e Marçal (1968), que utilizaram iterações do tipo Newton
para contornarem os possíveis erros nas aproximações incrementais; Zienkiewicz
(1971), que apresentou uma modificação no método de Newton-Raphson, fazendo com
que a matriz de rigidez só fosse atualizada a cada passo de carga.
Diversos trabalhos têm sido publicados apresentando diferentes estratégias de
controle automático do processo incremental, bem como diferentes estratégias de
iteração. Utilizando um ‘parâmetro de rigidez corrente’ como indicador do grau de não-
linearidade do sistema, Bergan et al. (1978) e Bergan (1980) suprimiram as iterações de
equilíbrio nas zonas críticas da trajetória, até os pontos limites serem atravessados; os
trabalhos de Bergan et al. (1978) e Heijer e Rheinbold (1981) forneceram diferentes
estratégias de incremento de carga.
Batoz e Dhatt (1979) apresentaram uma técnica na qual o ciclo iterativo é
realizado não à carga constante, mas a deslocamento constante, o que permite se obter
os pontos limites de carga mas não os de deslocamento; Riks (1979) apresentou um
método, baseado no parâmetro comprimento de arco ∆l, capaz de calcular pontos limites
de carga e de deslocamento com a introdução de um parâmetro que controla o progresso
dos cálculos ao longo do caminho de equilíbrio; Meek e Tan (1984) apresentaram um
resumo das principais técnicas para se ultrapassar os pontos limites, das quais a técnica
do comprimento de arco foi reconhecida como uma das mais eficientes. Contribuíram
com essa técnica: Riks (1972 e 1979), Ramm (1981), Schweizerhof e Wriggers (1986) e
Crisfield (1981, 1991 e 1997).
Yang e Kuo (1994) introduziram estratégias de incremento de carga e iteração
baseadas em relações de restrição para as quais é definido um parâmetro generalizado,
8
Krenk (1993 e 1995) elaborou uma nova estratégia de iteração, introduzindo duas
condição de ortogonalidade: a primeira entre o vetor de cargas residuais e o incremento
de deslocamento e a outra entre o incremento de forças internas e o vetor de
deslocamentos iterativos.
Crisfield (1997) introduziu procedimentos numéricos que permitem avaliar com
precisão os pontos críticos existentes, e obter as trajetórias de equilíbrio secundárias.
Silveira et al. (1999a-b) forneceram uma metodologia geral de solução de
sistemas de equações algébricas não-lineares que, num contexto computacional pode ser
resumida em duas partes: (i) a partir de uma dada configuração de equilíbrio da
estrutura é calculada uma solução incremental inicial; (ii) em seguida, essa solução é
corrigida com iterações do tipo Newton até ser atingida a nova configuração de
equilíbrio. Nesses dois trabalhos diversas estratégias de iteração e incremento de carga
foram testadas. Utilizando a mesma metodologia, Rocha (2000), em sua Dissertação de
Mestrado, vem realizando um estudo comparativo de diversas estratégias de iteração e
incremento de carga através da análise de vários exemplos numéricos de sistemas
estruturais.
2SOLUÇÃO NÃO-LINEAR
2.1 – INTRODUÇÃO
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2.5.2 – Iteração usando Deslocamento Generalizado
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2.5.3 – Iteração usando Resíduo Ortogonal
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