- #1
octol
- 61
- 0
I have a question over a thing that I've been thinking about lately, and that is why is it that
[tex] F = -\frac{dV}{dx} [/tex]
where [tex]V[/tex] is a potential? I don't remember seeing an explanation for that during my course in classical mechanics.
[tex] F = -\frac{dV}{dx} [/tex]
where [tex]V[/tex] is a potential? I don't remember seeing an explanation for that during my course in classical mechanics.