Lagrange Densities: Intuitive Understanding

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SUMMARY

The discussion focuses on the transition from the Lagrangian of a point particle to the Lagrangian of extended objects, specifically strings. It emphasizes that the Lagrangian of a string is derived by integrating the Lagrange density over its infinitesimal parts, analogous to summing forces to determine total force. The kinetic energy of the string is the sum of the kinetic energies of its segments, while the potential energy is represented by the expression ##S(\ell-\ell_0)##, where ##S## denotes the string's tension. This establishes a clear connection between classical mechanics and field theories.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with the concept of Lagrange density
  • Basic knowledge of kinetic and potential energy
  • Experience with Newton's equations of motion
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  • Study the derivation of Lagrange densities in field theory
  • Explore the application of the superposition principle in Lagrangian mechanics
  • Investigate the relationship between tension and potential energy in strings
  • Learn about the transition from discrete to continuous systems in physics
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Physicists, students of theoretical mechanics, and anyone interested in understanding the principles of Lagrangian dynamics applied to extended objects like strings.

Higgsono
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I'm a little confused when we transition from the Lagrangian of a point particle to consider Lagrangian of objects with dimension bigger then zero. For instance, the Lagrangian of a string is the sum of the Lagrangians for each infinitesimal part of the object. which means we are integrating over a Lagrange density to get the full Lagrangian. Intuitively I'm not sure why this works. But I think that it's analogous to the situation when we sum up all the forces on the object to determine the total force on the object.

In the case of solving Newton's equation of motion, the superposition principle for the forces seems intuitive, but it is not obvious that it carries over so that the superposition principle applies to the action as well.
 
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The Lagrangian is kinetic - potential energy. You are just finding those quantities for a string. It should be quite clear that the kinetic energy is the sum of the kinetic energies of each part of the string and that the potential of the string is ##S(\ell-\ell_0)##, where ##S## is the tension in the string.
 

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