# Where is potential energy in relativistic formula of energy?

by ndung200790
Tags: energy, formula, potential, relativistic
 Emeritus Sci Advisor PF Gold P: 5,598 You may be more likely to get helpful responses to your posts if you make them easier to read by marking the math up in LaTeX. Here is an example: $\sqrt{x^2+y^2}=1$. To see how I did that, click the QUOTE button on my post.
The question has to be more specific: what kind of force? Because if it is gravity, you need to do some GR and it's not exactly a potential anymore. If it's EM, the potential is a 4-vector: $(\phi, \mathbf{A})$, where $\phi$ is the scalar potential and $\mathbf{A}$ the vector potential. The Hamiltonian in this case is:
$$H = \sqrt{m^2 c^4 + \left(\mathbf{p} - e\mathbf{A}\right)^2 c^2} + e\phi$$
 P: 25 Where is potential energy in relativistic formula of energy? If it's gravity, then both potential and kinetic energy are generalised as (letting c=1):$-m\frac{d\tau}{dt}$where$d\tau^2=g_{\mu\nu}dx^{\mu}dx^{\nu}$We can see this clearly when we assume spherical symmetry and consider the Newtonian limit:$-m\frac{d\tau}{dt}=-m\sqrt{\frac{g_{tt}dt^2+g_{mm}(dx^m)^2}{dt^2}}$$=-m\sqrt{g_{tt}-\dot{x}^2}$$=-m\sqrt{1-\frac{2GM}{r}-\dot{x}^2}$$\approx-m+\frac{GMm}{r}+\frac{1}{2}m\dot{x}^2$And given that the action in a gravity well is$-m\int{d\tau}=0$then we recover the non-relativistic$E=\Delta{U}+KE$