Adding a variable to a Lagrangian

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MyoPhilosopher
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Homework Statement
$$ L = m\vec{\dot r}$$
Relevant Equations
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Would the following: $$ L = m(\vec{\dot r + \vec v})$$ (constant velocity added to above eq.)
lead to equivalent euler-lagrange equations due to the fact that the ratio of T and V is unaffected by an increase in constant velocity?
And would this be an example of energy conservation?
 
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actually the Lagrange equations do not care even if you add
$$\frac{d}{dt}f(t,\boldsymbol r)=\frac{\partial f}{\partial t }+\Big(\frac{\partial f}{\partial \boldsymbol r},\boldsymbol{\dot r}\Big)$$
 
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TSny said:
##L## should have dimensions of energy, not momentum.

##L## can be expressed in terms of ##T## and ##V##.
wrobel said:
actually the Lagrange equations do not care even if you add
$$\frac{d}{dt}f(t,\boldsymbol r)=\frac{\partial f}{\partial t }+\Big(\frac{\partial f}{\partial \boldsymbol r},\boldsymbol{\dot r}\Big)$$
What exactly does adding constant velocity do? Would is simply increase the r_dot vectors equally and therefore not affect the equations of motion?
 
TSny said:
##L## should have dimensions of energy, not momentum.

##L## can be expressed in terms of ##T## and ##V##.
I should have squared my second term, would this be appropriate $$ L = {m(\vec{\dot r + \vec v})}^2$$
 
MyoPhilosopher said:
What exactly does adding constant velocity do? Would is simply increase the r_dot vectors equally and therefore not affect the equations of motion?
Adding a constant velocity is effectively doing a Galilean boost, i.e., transforming to a coordinate system that moves at constant velocity relative to your original coordinate system.

The difference between the Lagrangians is ##m (\vec v \cdot \dot{\vec r} + v^2/2) = \frac d{dt}(\vec v \cdot \vec r + v^2 t/2)##. Thus, as per #4, the equations of motion are invariant under this transformation (which actually is the transformation ##\vec r \to \vec r + \vec v t##).
 
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Orodruin said:
Adding a constant velocity is effectively doing a Galilean boost, i.e., transforming to a coordinate system that moves at constant velocity relative to your original coordinate system.

The difference between the Lagrangians is ##m (\vec v \cdot \dot{\vec r} + v^2/2) = \frac d{dt}(\vec v \cdot \vec r + v^2 t/2)##. Thus, as per #4, the equations of motion are invariant under this transformation (which actually is the transformation ##\vec r \to \vec r + \vec v t##).

Ahhh thank you that clarified it elegantly!