Lagrange equation: when exactly does it apply?

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SUMMARY

The Lagrange equation applies to systems with holonomic constraints, but it can also accommodate non-conservative forces, such as friction, as indicated by the modified Euler-Lagrange equation: $$\frac{\partial L }{\partial q_j} - \frac{d}{d t} \frac{\partial L }{\partial \dot{q_j}} = Q_j$$. The discussion emphasizes that the kinetic energy, represented as T, can have explicit position dependence, particularly in spherical or polar coordinates. Readers are encouraged to consult Goldstein's "Classical Mechanics" for deeper insights into these concepts.

PREREQUISITES
  • Understanding of the Euler-Lagrange equation
  • Familiarity with holonomic and non-holonomic constraints
  • Knowledge of kinetic energy and its dependence on position
  • Basic principles of classical mechanics as outlined in Goldstein's "Classical Mechanics"
NEXT STEPS
  • Study the derivation and applications of the Euler-Lagrange equation
  • Explore the implications of holonomic versus non-holonomic constraints in mechanics
  • Investigate the role of generalized forces in the modified Lagrange equation
  • Examine examples of kinetic energy dependence on position in various coordinate systems
USEFUL FOR

Students and professionals in physics, particularly those focusing on classical mechanics, as well as researchers interested in advanced applications of the Lagrange equation in dynamic systems.

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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