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

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SUMMARY

The discussion centers on the impact of substituting functions into a Lagrangian on the equations of motion for a mechanical system with l + m degrees of freedom. The new Lagrangian, M(β, ẋβ, t) = L(f(t), β, ẋf(t), ẋβ, t), accurately describes the motion of the system when the first l degrees of freedom are constrained by an external force represented by f(t). It is confirmed that deriving equations from M will yield the correct motion for the constrained system, while substituting f(t) directly into the original equations of motion from L is not valid.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with degrees of freedom in mechanical systems
  • Knowledge of constraints in dynamical systems
  • Basic calculus, particularly differentiation with respect to time
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  • Study the derivation of equations of motion from Lagrangians in classical mechanics
  • Explore the concept of constraints in Lagrangian systems
  • Learn about the implications of substituting functions in Lagrangian formulations
  • Investigate the role of external forces in mechanical systems
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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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