1

My question is simple.

  1. In the classical mechanics, we know the least action principle does the variation on the action $$ S = \int (T-V) dt , $$ where $T$ is the kinetic term and $V$ is the potential term, to give the classical equations of motion.

So why the least action principle extremizes (minimizes or maxmizes) this quantity

$$T-V = H- 2V = E-2V =2 T- H = 2T-E?$$ Here I also denote $H$ as Hamiltonian. And $E$ as the energy of the system. In this regard, the $E$ is conserved, but not extremized. But $$E-2V =2T-E$$ is extremized!

  1. For example, if we write down the $(T-V)$ for a free falling object under constant gravitational acceleration $g$, we have $$T-V = \frac{1}{2} m \dot{y}^2 - m g y = E -2 m g y = m \dot{y}^2 -E$$ with $E=\frac{1}{2} m \dot{y}^2 + m g y$ is conserved.

What is the physical significance of this $T-V$?

(Provide good physical or math reasons.)

I know how to derive equations of motion. I am asking a transparent way to understand why $T-V$ is in extremization.

I suppose the extremization may minimizes or maximizes the action. (Not necessarily minimization, correct?) Do we have both examples of

  • The equations of motion minimize the action?

  • The equations of motion maximize the action?

Qmechanic
  • 220,844

0 Answers0