How Does Substituting Functions into a Lagrangian Affect Equations of Motion?

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Discussion Overview

The discussion centers on the implications of substituting functions into a Lagrangian for a mechanical system with multiple degrees of freedom. Participants explore whether the modified Lagrangian accurately describes the motion of the original system when certain degrees of freedom are constrained by an external force.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents a mechanical system with degrees of freedom described by a Lagrangian and questions if substituting a known function into a new Lagrangian yields correct equations of motion.
  • Another participant references the Euler-Lagrange equations and suggests that the new Lagrangian would yield the correct equations corresponding to the remaining degrees of freedom.
  • A different participant raises a concern about potential extra terms arising from the time derivative of the substituted function, indicating uncertainty about the implications of this substitution.
  • Some participants assert that the modified Lagrangian correctly describes the constrained system, emphasizing that it is a common practice to impose constraints after formulating the Lagrangian.
  • There is a caution expressed that substituting the function into the original equations of motion derived from the initial Lagrangian may not be valid.

Areas of Agreement / Disagreement

Participants generally agree that the modified Lagrangian can describe the constrained system, but there is disagreement regarding the validity of substituting the function into the original equations of motion. The discussion remains unresolved on the implications of extra terms from the substitution.

Contextual Notes

Participants note the lack of rigorous proofs for some claims and the potential for additional terms arising from derivatives, indicating that assumptions about the nature of the functions and constraints may not be fully addressed.

Petr Mugver
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Suppose I have a mechanical system with l + m degrees of freedom and an associated lagrangian

L(\alpha,\beta,\dot{\alpha},\dot{\beta},t)

where \alpha\in\mathbb{R}^l and \beta\in\mathbb{R}^m.
Now suppose I have a known \mathbb{R}^l-valued function f(t) and define a new lagrangian

M(\beta,\dot{\beta},t)=L(f(t),\beta,\dot{f}(t), \dot{\beta},t)

Do the equations that derive from M correctly describe the motion of the initial mechanical system, where the first l degrees of freedom are constrained to the motion f(t) (by means of an external force)?
 
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\frac{\partial L}{\partial q} = \frac{d}{dt} \frac{\partial L}{\partial \dot{q} }
where q is anyone of the coordinates of \alpha or \beta (i.e. there are l+m separate equations).
From this, I would assume that M(\beta , \dot{\beta} , t) would be correct, because this simply gives the m equations, which correspond to \beta.
(I know I've not done a rigorous proof or anything, but this seems to make sense to me).
 
BruceW said:
\frac{\partial L}{\partial q} = \frac{d}{dt} \frac{\partial L}{\partial \dot{q} }
where q is anyone of the coordinates of \alpha or \beta (i.e. there are l+m separate equations).
From this, I would assume that M(\beta , \dot{\beta} , t) would be correct, because this simply gives the m equations, which correspond to \beta.
(I know I've not done a rigorous proof or anything, but this seems to make sense to me).

Uhm, please don't let me write the formula, but when you take the derivative with respect to t of the momentum dM/dv, don't you get extra terms due to f(t) and df(t)/dt?
 
Do the equations that derive from M correctly describe the motion of the initial mechanical system, where the first l degrees of freedom are constrained to the motion f(t) (by means of an external force)?
Yes, this is correct. In fact it's done all the time: write down T and V as if the particles were entirely free, and then impose the constraints on them. The Lagrangian M you get from this will describe the motion of the constrained system.

What you cannot do is the other way around: trying to substitute f(t) into the equations of motion you originally derived from L.
 
Bill_K said:
Yes, this is correct. In fact it's done all the time: write down T and V as if the particles were entirely free, and then impose the constraints on them. The Lagrangian M you get from this will describe the motion of the constrained system.

What you cannot do is the other way around: trying to substitute f(t) into the equations of motion you originally derived from L.

Yes, it sounds so obvious. I feel stupid now... :)
 

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