Functional variation of Lagrangian densities

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SUMMARY

The discussion focuses on the treatment of a scalar field φ and its derivatives as independent variables in the context of deriving stationary solutions for the action in Lagrangian mechanics. It establishes that this approach allows for a comprehensive formulation of the Lagrangian, which is essential for transitioning to Hamiltonian formalism and accurately describing dynamics. The Lagrangian is defined as a function of positions and velocities, where kinetic energy (KE) incorporates time derivatives of position, while potential energy (PE) depends solely on position and time. The fundamental variational principle of Hamilton is emphasized as a means to identify physically realizable mechanical states through the solutions of Lagrange equations.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with Hamiltonian formalism
  • Knowledge of variational principles in physics
  • Basic concepts of scalar fields in theoretical physics
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  • Study the derivation of Lagrange equations from the action principle
  • Explore Hamiltonian mechanics and its applications
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The discussion is beneficial for theoretical physicists, graduate students in physics, and anyone interested in advanced mechanics and field theory concepts.

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Why do we treat a scalar field phi and its derivatives as being independent when trying to find a stationary solution for the action?

Doesn't that give too general solutions?

Where does the restriction that (d_mu phi) is dependent on phi come back in?
 
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That's the idea. We take things as general as possible. The Lagrangian needs to be a function of positions and velocities treated as independent variables as to allow the passing to the Hamiltonian formalism on one hand and account for the correct description of dynamics on the other. I mean we usually see the lagrangian as the KE-PE function and the KE part involves time derivatives of position (generalized velocities), while the PE part is allowed to depend only on "x" and "t", and not on [itex]\frac{dx}{dt}[/itex].

Setting things so general we have to use the fundamental variational principle of Hamilton which selects the physically realizable mechanical states,which are of course the solutions of Lagrange equations.

Daniel.
 

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