Prove the Langrangian is not unique

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The discussion centers on proving the non-uniqueness of the Lagrangian by showing that a modified Lagrangian L' satisfies Lagrange's equations under certain conditions. A participant expresses difficulty in solving the problem through direct substitution, having only found a solution using the action integral. It is noted that the function F must not depend on velocity; otherwise, the two Lagrangians would not be equivalent. The theorem referenced states that a function satisfies Lagrange's equations identically if it is the total time derivative of a function F that depends only on position and time. The conversation emphasizes the importance of the conditions under which L' can be shown to satisfy Lagrange's equations.
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Question:
If L is a Lagrangian for a system of n degrees of freedom satisfying Lagrange's equations show by direct substitution that

http://qlx.is.quoracdn.net/main-74d090d14ee4fea0.png

also satisfies Lagrange's equations where F is any arbitrary but differentiable function of its arguments.
Attempt at a solution:
I'm not really sure how to solve this problem by direct substitution; I found a way to do it using the action integral but not direct substitution. Any clues or help on how to approach the problem?
 
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Use L' as the new lagrangian in Lagrange's equation.
Does L' satisfy that equation? Under what condition?
 
I got that L' satisfies that equation when the derivative for Lagrange's equation of F is 0.
 
You should probably show your work.
You can use the LaTeX button below to help you typeset your equations.
 
I don't know how to write LaTeX
11251701_10153310866401660_2140605752_n.jpg
 
It's me said:
Question:
If L is a Lagrangian for a system of n degrees of freedom satisfying Lagrange's equations show by direct substitution that

http://qlx.is.quoracdn.net/main-74d090d14ee4fea0.png

also satisfies Lagrange's equations where F is any arbitrary but differentiable function of its arguments.

Your question is wrong. The function F can not depend on the velocity \dot{q}(t). If it does, then d F /d t will depend (at least linearly) on the acceleration \ddot{q}(t). This in turns mean that the two Lagrangians are not equivalent to each other. So, try to solve the exercise for the function F(t) = F( q(t) , t ).

This is one part of well know theorem which states

A function \Lambda of q(t), \dot{q}(t) and t satisfies Lagrange’s equations identically (i.e., independent of the q_{a}(t)) if, and only if, it is the total time derivative d F / dt of some function F ( q(t) , t ).
 
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