m(v⃗×v⃗)r\frac{m(\vec{v} \times \vec{v})}{r}rm(v×v)
−m(v⃗×v⃗)r-\frac{m(\vec{v} \times \vec{v})}{r}−rm(v×v)
m(ω⃗⋅ω⃗)r⃗m(\vec{\omega} \cdot \vec{\omega}) \vec{r}m(ω⋅ω)r
−m(ω⃗⋅ω⃗)r⃗-m(\vec{\omega} \cdot \vec{\omega}) \vec{r}−m(ω⋅ω)r