What is the Principle of Least Action?

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SUMMARY

The discussion centers on demonstrating the Principle of Least Action using the Lagrangian for a mass in a uniform gravitational field, expressed as L = (1/2)m˙y² + mgy. Participants suggest approaches to prove that the action is minimized for the true motion of the particle, including perturbing the equation of motion and applying calculus of variations. The consensus emphasizes that the action for any perturbed motion must exceed that of the true motion, reinforcing the principle's validity.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with the concept of action in physics
  • Basic knowledge of calculus, particularly derivatives
  • Introduction to calculus of variations (recommended for deeper insight)
NEXT STEPS
  • Study the derivation of the Lagrangian in classical mechanics
  • Explore perturbation methods in physics
  • Learn about calculus of variations and its applications
  • Investigate examples of the Principle of Least Action in different physical systems
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Students of physics, particularly those studying classical mechanics, and educators looking to enhance their understanding of the Principle of Least Action and its applications in motion analysis.

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Homework Statement


The Lagrangian of a mass in a uniform gravitational field can be written as follows: L = \frac{1}{2}m\dot{y}^2 + mgy

Consider all differentiale functions y(t) such that y(t1) = y1 and y(t2) = y2 where y1 and y2 are fixed values. Show that the action is a minimum for the function defining the true motion.


Homework Equations



I believe this simply an 'example' of prooving the principle of least action.

The Attempt at a Solution



I am wondering where to start. I derived the equation of true motion of the particle. Should I know plus in the given Lagrangian to the action integral and then then add a pertubation to the equation of true motion and then plug THAT into the action and show that the action of the perturbed equation of motion must be greater then the action of the original?

Thanks guys!
 
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Your idea is one way of doing it.

Another way would be to find the function that minimizes the action using calculus of variations, and see that it is the same as the true motion which you derived indepedently.
 
We have not been taught calculus of variations yet, though I may look into that. Thanks!
 

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