- #1
Lightf
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Homework Statement
Consider the following Lagrangian of a relativistic particle moving in a D-dim space and interacting with a central potential field.
$$L=-mc^2 \sqrt{1-\frac{v^2}{c^2}} - \frac{\alpha}{r}\exp^{-\beta r}$$
...
Find the velocity v of the particle as a function of p and r.
Homework Equations
Lagrange's Equations of motion
$$\frac{d}{dt}(\frac{dL}{dv})= \frac{dL}{dr}$$
The Attempt at a Solution
$$\frac{dL}{dr} = \frac{\alpha \exp^{-\beta r}(r+1)}{r^2}$$
$$\frac{dL}{dv} \equiv p = \frac{mc^2 v}{\sqrt{1-\frac{v^2}{c^2}}}$$
$$\frac{d}{dt}(\frac{mc^2 v}{\sqrt{1-\frac{v^2}{c^2}}}) = \frac{\alpha \exp^{-\beta r}(r+1)}{r^2}$$
I am not sure what to do next. If I try to differentiate the left side I get
$$mc^2 \dot{v}(v^2(1-\frac{v^2}{c^2})^{-\frac{3}{2}} + (1-\frac{v^2}{c^2})^{-\frac{1}{2}} ) = \frac{\alpha \exp^{-\beta r}(r+1)}{r^2}$$
Which seems very hard to integrate.. Any ideas to find v easier?