Abstract
An energy principle to find the equations of motion is outlined within the scope of continuum classical mechanics and compared with the very useful and widely applied Hamilton's Principle. It is shown that to obtain convenient results by means of the latter principle, a strong restriction on the variations of the functions of interest must be accepted. Furthermore, such restrictions are confronted with the ones that, at the same time, derive from the manipulation of the principle herein proposed. Two illustrative examples are also included.
Get full access to this article
View all access options for this article.
