Lagrange equation: when exactly does it apply?

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Discussion Overview

The discussion revolves around the application of the Lagrange equation, specifically the Euler-Lagrange equation, in various contexts. Participants explore the conditions under which the equation applies, the nature of constraints, and the implications of generalized forces, including non-conservative forces like friction.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the Lagrange equation applies only to holonomic constraints and how constraining forces affect this classification.
  • Another participant clarifies that they are discussing the Euler-Lagrange equation and raises questions about the modified equation involving generalized forces, seeking conditions for its application.
  • A participant inquires whether the partial derivative of kinetic energy with respect to generalized coordinates can ever equal zero, suggesting that there may be cases of explicit dependence on position.
  • Another participant agrees that kinetic energy can depend on position, providing an example in spherical coordinates.
  • One participant references an external paper as a potential resource for further clarification on the topic.
  • A later reply suggests that revisiting specific chapters in Goldstein's book may help answer the initial questions posed.

Areas of Agreement / Disagreement

Participants express differing views on the conditions for applying the Lagrange equation and the nature of kinetic energy dependence, indicating that multiple competing perspectives remain without a clear consensus.

Contextual Notes

Participants note that the discussions involve assumptions about constraints and generalized forces, and there are unresolved questions regarding the derivation and application of the modified Euler-Lagrange equation.

Nikitin
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Hi! Does the Lagrange equation ONLY apply when the constraints are holonomic? What about the constraining forces acting on the system (i.e. normal force, or other perpendicular forces), do they make a system holonomic?

What about the Lagrange equation with the general force on the right hand side. I read in Goldstein that it can be, for instance, a non-conservative frictional force. Why? Where did that come from?
 
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BTW, I am talking about the Euler-Lagrange equation. This one, $$ \sum_j \frac{\partial L }{\partial q_j} - \frac{d}{d t} \frac{\partial L }{\partial \dot{q_j}} = 0$$ in case there was any confusion.

But what is up with the modified equation, ##\frac{\partial L }{\partial q_j} - \frac{d}{d t} \frac{\partial L }{\partial \dot{q_j}} = Q_j## ? When does this apply to a system, and for which generalized forces ##Q_j##s? It was not derived in Goldstein's book, just given.
 
Another question, if somebody wants to answer: does ##\frac{\partial T}{\partial q_j}##, where ##T## is the kinetic energy of the system, always equal zero? Or do there exist situations where the kinetic energy has an explicit dependence on position?

It might seem like a strange question because kinetic energy is defined using total velocity, but I ask because one form of Lagrange's equation is ##\frac{d}{dt} \frac{\partial T}{\partial \dot{q_j}} - \frac{\partial T}{\partial q_j} = Q_j##.
 
Nikitin said:
Another question, if somebody wants to answer: does ##\frac{\partial T}{\partial q_j}##, where ##T## is the kinetic energy of the system, always equal zero? Or do there exist situations where the kinetic energy has an explicit dependence on position?

It certainly can, in spherical coordinates (or polar) you have position dependence in the kinetic term.
 
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Check http://physics.clarku.edu/courses/201/sreading/AJP73_March2005_265-272.pdf paper out. Does that help answer your questions?
 
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I hate to answer your question this way, but if you reread Goldstein chapter 1 and 2 enough, you will answer your questions. This was true for me.
 

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