Classical Dynamics of Particles and Systems · Problem 1-32

Newtonian Mechanics—Single Particle — Marion & Thornton

Physics — Mechanics · vector-calculus-integration

Problem

Show that ∫(2ar⋅r˙+2br˙⋅r¨) dt=ar2+br˙2+const.\int(2a\mathbf{r} \cdot \dot{\mathbf{r}} + 2b\dot{\mathbf{r}} \cdot \ddot{\mathbf{r}})\,dt = ar^2 + b\dot{r}^2 + \text{const.} where r\mathbf{r} is the vector from the origin to the point (x1,x2,x3)(x_1, x_2, x_3). The quantities rr and r˙\dot{r} are the magnitudes of the vectors r\mathbf{r} and r˙\dot{\mathbf{r}}, respectively, and aa and bb are constants.

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