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Modelling with PDEs

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Resumo:Taking in consideration the audience, we explore a prospective point of view. We intend to comment on some qualitative aspects and issues concerning the mathematical work of modelization with Partial Differential Equations (PDEs). A class of evolution PDEs: \pa_t u+div f(u)=\eps div b(u,\grad u)+\del div \pa_(\xi) c(u,\grad u), which include generalized Korteweg-de Vries-Burgers equation (when \xi is a space variable) and Benjamin-Bona-Mahony-Burgers equation (when \xi is the time variable), or that of \pa_t u+div f(u)=\del div c(u,\grad u), which can present unexpected dissipative properties. As "\eps,\del-parameters tend to zero we can have failure (i.e., no limit solution at all for \del > O(\eps^\gamma)) or reliability (with different limits: classical-entropy weak-solutions inside an integrity region \del < O(\eps^\gamma) and nonclassicalentropy weak-solutions along \del = O(\eps^\gamma)), according to the \gamma-balance of \eps,\del-strengths and to the ratio between the growths of the b-dissipation and c-dispersion.
Autores principais:Correia, Joaquim M.C.
Assunto:Modelling Partial Differential Equations Korteweg-de Vries-Burgers equation Benjamin-Bona-Mahony-Burgers equation failure reliability integrity classical-entropy weak-solutions nonclassicalentropy weak-solutions dissipation dispersion
Ano:2015
País:Portugal
Tipo de documento:palestra
Tipo de acesso:acesso restrito
Instituição associada:Universidade de Évora
Idioma:inglês
Origem:Repositório Científico da Universidade de Évora
Descrição
Resumo:Taking in consideration the audience, we explore a prospective point of view. We intend to comment on some qualitative aspects and issues concerning the mathematical work of modelization with Partial Differential Equations (PDEs). A class of evolution PDEs: \pa_t u+div f(u)=\eps div b(u,\grad u)+\del div \pa_(\xi) c(u,\grad u), which include generalized Korteweg-de Vries-Burgers equation (when \xi is a space variable) and Benjamin-Bona-Mahony-Burgers equation (when \xi is the time variable), or that of \pa_t u+div f(u)=\del div c(u,\grad u), which can present unexpected dissipative properties. As "\eps,\del-parameters tend to zero we can have failure (i.e., no limit solution at all for \del > O(\eps^\gamma)) or reliability (with different limits: classical-entropy weak-solutions inside an integrity region \del < O(\eps^\gamma) and nonclassicalentropy weak-solutions along \del = O(\eps^\gamma)), according to the \gamma-balance of \eps,\del-strengths and to the ratio between the growths of the b-dissipation and c-dispersion.

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