In physics, Hamilton's principle is William Rowan Hamilton's formulation of the principle of stationary action (see that article for historical formulations). It states that the dynamics of a physical system is determined by a variational problem for a functional based on a single function, the Lagrangian, which contains all physical information concerning the system and the forces acting on it. The variational problem is equivalent to and allows for the derivation of the differential equations of motion of the physical system. Although formulated originally for classical mechanics, Hamilton's principle also applies to classical fields such as the electromagnetic and gravitational fields, and has even been extended to quantum mechanics, quantum field theory and criticality theories.
Read more about Hamilton's Principle: Mathematical Formulation, Hamilton's Principle Applied To Deformable Bodies, Comparison With Maupertuis' Principle
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—Alexander Hamilton (1757–1804)
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—Charles Dickens (1812–1870)