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Functionals:
Lagrangian Mechanics
Lagrange's equations





Lagrange equation


Here is the Euler-Lagrange equation:

d[∂f/∂y']/dx = ∂f/∂y .

In Classical Mechanics, this equation takes the general expression:

d[∂L/∂qi']/dt = ∂L/∂qi .

q(t) is the trajectory of a system of one particle of M degrees of freedom described by the configurational coordinates q(t) = (q1(t), q2(t), . . . qM(t)) with respect to the time t. In case of N classical particles holds M = 3N.

The function L is the Lagrangian; function of the variable positions q, the velocities q', and the time t related to the system.

L = L(q(t), q'(t), t) = KE(i) - PE(i) .

KE(i) and PE(i) are respectively the kinetic energy and the potential energy of the system.

This formula is expressed as:

L(q(t), q'(t), t) = (1/2)m q'i2 - U(q1(t), q2(t), . . . qM) .

The Lagrangian equation takes then the following expression:

m qi" = ∂U/∂qi
i = 1, 2, ..., M


In Classical Mechanics, Lagrange's equation is:



More simplified, it reads:






  


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