Motion equation of a finite dynamic elastic plane lineal element plane lineal element
A linear finite element with constant cross section can take any orientation in the plane and its ends or nodes bind it to the rest of the elements. The kinetic (T) and potential (V) energy of a dynamic elastic element are the basis for the implementation of the Hamilton principle for the definition...
- Autores:
-
G Hossne, Américo
- Tipo de recurso:
- Fecha de publicación:
- 2010
- Institución:
- Universidad EAFIT
- Repositorio:
- Repositorio EAFIT
- Idioma:
- spa
- OAI Identifier:
- oai:repository.eafit.edu.co:10784/14482
- Acceso en línea:
- http://hdl.handle.net/10784/14482
- Palabra clave:
- Hamilton Principle
Dynamic Elastic Flat Linear Finite Element
Four-Bar Elastic Mechanisms
Lagrangian
Mass Matrix
Rigidity Matrix And Gyroscopic Matrix
Principio De Hamilton
Elemento Finito Lineal Plano Elástico Dinámico
Mecanismos Elásticos De Cuatro Barras
Lagrangiana
Matriz De Masas
Matriz De Rigideces Y Matriz Giroscópica
- Rights
- License
- Copyright (c) 2010 Américo G Hossne