Logarythmic
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I have showed that if the integrand f in the variational problem
\delta (\int f dx ) = 0
does not depend explicitly on the independent variable x, i.e. satisfies f = f(y, \dot{y}), then the Euler equation can be integrated to
\dot{y} \frac{\partial f}{\partial \dot{y}} - f = const.
How can I give an interpretation of this constant for the case that f = L is the Lagrangian and x = t is the time?
\delta (\int f dx ) = 0
does not depend explicitly on the independent variable x, i.e. satisfies f = f(y, \dot{y}), then the Euler equation can be integrated to
\dot{y} \frac{\partial f}{\partial \dot{y}} - f = const.
How can I give an interpretation of this constant for the case that f = L is the Lagrangian and x = t is the time?