International audienceAn alternative derivation of the equation of motion of a charged point particle from Hamilton's principle is presented. The variational principle is restated as a Bolza problem of optimal control, the control variable u i , i = 0, …, 3, being the 4-velocity. The trajectory ( s) i and 4-velocity ū i ( s) of the particle is an optimal pair, i.e., it furnishes an extremum to the action integral. The pair ( , ū) satisfies a set of necessary conditions known as the maximum principle. Because of the path dependence of proper time s, we are concerned with a control problem with a free end point in the space of coordinates (s, x 0 , …, x 3 ). To obtain the equation of motion, the transversality condition must be satisfied ...
The transport and distribution of charged particles are crucial in the study of many physical and bi...
Abstract We give a geometric interpretation for the principle of stationary action in classical Lagr...
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I present an intuitive answer to an often asked question: why is the integrated difference K-U betwe...
DoctoralThis note presents different descriptions of the equations of motion of a charged particle s...
The Lagrange formalism on dissipative systems is extended by a new variational principle extremum of...
These lecture notes are concerned with the derivation of the fluid mechanics equations via Hamilton'...
A simple mathematical procedure is introduced which allows redefining in an exact way divergent inte...
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The Classical Newton-Lagrange equations of motion represent the fundamental physical law of mechanic...
The equations of motion of a point particle interacting with charge symmetrical mesons are deduced o...
We show that within the relativistic dynamics of a particle the Hamilton's action yields the mechani...
A new variational principle extremum of full action is proposed, which extends the Lagrange formalis...
We develop a Hamiltonian formalism that can be used to study the particle dynamics near stable equil...
AbstractA differential action principle written as follows, δq = − ∂δW∂p; δp = ∂δW∂q, is obtained by...
The transport and distribution of charged particles are crucial in the study of many physical and bi...
Abstract We give a geometric interpretation for the principle of stationary action in classical Lagr...
An unsolved problem of classical mechanics and classical electrodynamics is related to the search of...
I present an intuitive answer to an often asked question: why is the integrated difference K-U betwe...
DoctoralThis note presents different descriptions of the equations of motion of a charged particle s...
The Lagrange formalism on dissipative systems is extended by a new variational principle extremum of...
These lecture notes are concerned with the derivation of the fluid mechanics equations via Hamilton'...
A simple mathematical procedure is introduced which allows redefining in an exact way divergent inte...
This chapter investigates applications of the principles of analyticalmechanics developed in chapter...
The Classical Newton-Lagrange equations of motion represent the fundamental physical law of mechanic...
The equations of motion of a point particle interacting with charge symmetrical mesons are deduced o...
We show that within the relativistic dynamics of a particle the Hamilton's action yields the mechani...
A new variational principle extremum of full action is proposed, which extends the Lagrange formalis...
We develop a Hamiltonian formalism that can be used to study the particle dynamics near stable equil...
AbstractA differential action principle written as follows, δq = − ∂δW∂p; δp = ∂δW∂q, is obtained by...
The transport and distribution of charged particles are crucial in the study of many physical and bi...
Abstract We give a geometric interpretation for the principle of stationary action in classical Lagr...
An unsolved problem of classical mechanics and classical electrodynamics is related to the search of...