ABSTRACT
Much has been said and written on the calculus of variations, a traditional subject of mathematics, and the offered models have often been expressed in terms of minimality or maximality. The traditional methods (Euler-Lagrange equation , Hamiltonian formulation and Hamilton-Jacobi equation) and the direct methods are explained. The vectorial case of direct methods is then presented via the different notions of convexity and an existence result. Non-convex problems of the calculus of variations conclude this article: different envelopes, relaxation theorem and various examples.
Read this article from a comprehensive knowledge base, updated and supplemented with articles reviewed by scientific committees.
Read the article
INTRODUCTION
The calculus of variations is one of the classic subjects of mathematics. It has attracted many famous mathematicians. Before presenting the most important model case, we'll start with an informal discussion. In mathematics, physics, engineering or even economics or ecology, models are often expressed in terms of a minimality or maximality principle. This is precisely the central issue in calculating variations. For example, in mathematics, we may be interested in finding, under certain constraints, a curve of minimum length or a surface of minimum area. In physics, a typical example is the principle of least action; other examples will be given in more detail in this presentation. Conservation laws, which correspond mathematically to differential equations, are often derived from a variational principle. The solutions of the variational problem are then solutions of associated differential equations.
You do not have access to this resource.
Exclusive to subscribers. 97% yet to be discovered!
Already subscribed?
Log in!
Ongoing reading
Calculus of variations