Classical Dynamics of Particles and Systems · Problem 1-33

Newtonian Mechanics—Single Particle — Marion & Thornton

Physics — Mechanics · vector-calculus-integration

Problem

Show that ∫(r˙r−rr˙r2)dt=rr+C\int\left(\frac{\dot{\mathbf{r}}}{r} - \frac{\mathbf{r}\dot{r}}{r^2}\right)dt = \frac{\mathbf{r}}{r} + \mathbf{C} where C\mathbf{C} is a constant vector.

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