Differences
This shows you the differences between two versions of the page.
| Both sides previous revision Previous revision | Last revisionBoth sides next revision | ||
| 183_notes:ap_derivation [2014/11/20 18:06] – caballero | 183_notes:ap_derivation [2014/11/20 18:06] – caballero | ||
|---|---|---|---|
| Line 25: | Line 25: | ||
| $$\vec{\tau}_{net} = \dfrac{d}{dt}\left(\vec{r} \times \vec{p}\right) - m \underbrace{\vec{v} \times \vec{v}}_{=0}$$ | $$\vec{\tau}_{net} = \dfrac{d}{dt}\left(\vec{r} \times \vec{p}\right) - m \underbrace{\vec{v} \times \vec{v}}_{=0}$$ | ||
| - | And thus, we have the angular momentum principle in it' | + | And thus, we have the angular momentum principle in its derivative form, |
| $$\vec{\tau}_{net} = \dfrac{d}{dt}\left(\vec{r} \times \vec{p}\right)$$ | $$\vec{\tau}_{net} = \dfrac{d}{dt}\left(\vec{r} \times \vec{p}\right)$$ | ||