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

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Substituting functions into a Lagrangian can accurately describe the motion of a mechanical system when the first degrees of freedom are constrained by an external force. The new Lagrangian, defined as M(β, ẋβ, t) from L(α, β, ẋα, ẋβ, t), will yield correct equations of motion for the remaining degrees of freedom. It is common practice to derive the Lagrangian assuming free particles and then apply constraints. However, one cannot substitute the constraint function directly into the original equations of motion derived from the initial Lagrangian. This method ensures that the dynamics of the constrained system are properly represented.
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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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