- #1
kakarukeys
- 190
- 0
"There is some freedom as to what we choose for the Lagrangian in a given problem: We can add a constant, multiply by a constant, change the time scale by a multiplicative constant, or add the total time derivative ... Any of these transformations will lead to a Lagrangian that is perfectly satisfactory for describing the motion."
I could not verify the 3rd one. Why is it possible to change the time scale by a constant factor?
For example:
[tex]L = \frac{1}{2}m\dot{q}^2 - kqt[/tex]
The E-L equation is
[tex]m\ddot{q} + kt = 0[/tex]
If we modify the Lagrangian, multiplying all time by constant c
[tex]L = \frac{1}{2c^2}m\dot{q}^2 - ckqt[/tex]
The E-L equation is
[tex]m\ddot{q} + c^3kt = 0[/tex]
I could not verify the 3rd one. Why is it possible to change the time scale by a constant factor?
For example:
[tex]L = \frac{1}{2}m\dot{q}^2 - kqt[/tex]
The E-L equation is
[tex]m\ddot{q} + kt = 0[/tex]
If we modify the Lagrangian, multiplying all time by constant c
[tex]L = \frac{1}{2c^2}m\dot{q}^2 - ckqt[/tex]
The E-L equation is
[tex]m\ddot{q} + c^3kt = 0[/tex]