Classical Dynamics of Particles and Systems · Problem 1-27

Newtonian Mechanics—Single Particle — Marion & Thornton

Physics — Mechanics · vector-calculus

Problem

If r\mathbf{r} and r˙=v\dot{\mathbf{r}} = \mathbf{v} are both explicit functions of time, show that ddt[r×(v×r)]=r2a+(r⋅v)v−(v2+r⋅a)r\frac{d}{dt}[\mathbf{r} \times (\mathbf{v} \times \mathbf{r})] = r^2\mathbf{a} + (\mathbf{r} \cdot \mathbf{v})\mathbf{v} - (v^2 + \mathbf{r} \cdot \mathbf{a})\mathbf{r}

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