Is the Lagrangian a Function of Only Generalized Coordinates and Speed?

In summary, the discussion revolves around the proof of a Lagrangian being a function of just the generalized coordinates and speeds and not the generalized acceleration, which is typically assumed but not proven. The argument is that a variation of the action must result in a new "Euler-Lagrange" equation, which can be derived by considering the boundary terms from partial integrations. This equation must hold for any arbitrary variations, which leads to the conclusion that the Lagrangian is indeed independent of the generalized acceleration.
  • #1
pardesi
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0
Hmm how does one prove that a lagrangian is a function of just the generalized coordinates and the generalized speed and not the generalized "Accelaration"?
 
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  • #2
In general, one assumes that it does not depend on [itex]\ddot q_i[/itex] (with [itex]q_i[/itex] the generalized coordinates) because in most systems, it doesn't. But one cannot prove this independence, and indeed one can derive the Euler-Lagrange equations for a Lagrangian with does depend on them in the same way as usual.

One should check, however, that the "acceleration" is really independent, otherwise one cannot consider [itex]q[/itex] and [itex]\ddot q[/itex] as independent coordinates and one would have to impose a constraint (e.g. the original Euler-Lagrange equation for the Lagrangian which does not depend on the acceleration).

But in principle, I think this argument works:
Suppose we have a Lagrangian [itex]\mathcal L(q, \dot q, \ddot q)[/itex]. Then a variation of the action gives
[itex]\delta\left( \int \mathcal L \, \mathrm dt \right) = \int \left( \frac{\partial \mathcal L}{\partial q} \delta q + \frac{\partial \mathcal L}{\partial \dot q} \delta \dot q + \frac{\partial \mathcal L}{\partial \ddot q} \delta \ddot q \right) \, \mathrm dt. [/itex]
Using that [itex]\delta\dot q = \frac{d(\delta q)}{dt}[/itex], etc. we get by partial integration (once on the second term, twice on the third term)
[itex]\delta\left( \int \mathcal L \, \mathrm dt \right) = \int \left( \frac{\partial \mathcal L}{\partial q} - \frac{d}{dt} \frac{\partial \mathcal L}{\partial \dot q} + \frac{d^2}{dt^2} \frac{\partial \mathcal L}{\partial \ddot q} \right) \delta q \, \mathrm dt [/itex]
assuming that all the boundary terms from the partial integrations vanish. Now for this to vanish for arbitrary variations (under these conditions), the bracketed term must be zero and we find a new "Euler-Lagrange equation",
[tex]\frac{\partial \mathcal L}{\partial q} + \frac{d^2}{dt^2} \frac{\partial \mathcal L}{\partial \ddot q} = \frac{d}{dt} \frac{\partial \mathcal L}{\partial \dot q} [/tex]
 
  • #3
thanks!
hmm you i cud smell that but just wanted to confirm if i was missing out something
 

FAQ: Is the Lagrangian a Function of Only Generalized Coordinates and Speed?

What is a Lagrangian function?

A Lagrangian function, also known as a Lagrangian, is a mathematical function used in the field of Lagrangian mechanics to describe the dynamics of a physical system. It takes into account the kinetic and potential energies of the system and is used to derive the equations of motion.

What is the role of a Lagrangian function in physics?

A Lagrangian function plays a crucial role in physics, particularly in classical mechanics and quantum mechanics. It is used to describe the behavior of a physical system and derive the equations of motion. It is also used in the principle of least action, which states that the actual path of a system between two points is the one that minimizes the action, which is defined by the Lagrangian function.

How is a Lagrangian function different from a Hamiltonian function?

A Lagrangian function and a Hamiltonian function are both used in classical mechanics to describe the dynamics of a physical system. However, they differ in their approach - a Lagrangian function uses generalized coordinates and velocities to describe the system, while a Hamiltonian function uses generalized coordinates and momenta. In some cases, they can be related through a mathematical transformation.

Can a Lagrangian function be used in quantum mechanics?

Yes, a Lagrangian function can be used in quantum mechanics to describe the dynamics of a quantum system. However, it is more commonly used in classical mechanics. In quantum mechanics, the Lagrangian function is usually replaced by a quantum mechanical operator, known as the Hamiltonian operator, which is used to describe the state of a quantum system at a particular time.

How is a Lagrangian function derived?

A Lagrangian function is derived by taking the difference between the kinetic and potential energies of a physical system. It is typically based on the principle of least action, where the actual path of a system is the one that minimizes the action, which is defined by the Lagrangian function. The process of deriving a Lagrangian function involves identifying the generalized coordinates and velocities of the system, and then using these to write down the kinetic and potential energies.

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