v→=v→0+a→\overrightarrow{\mathrm{v}}=\overrightarrow{\mathrm{v}}_{0}+\overrightarrow{\mathrm{a}}v=v0+a
v2=v02+2a→⋅s→\mathrm{v}^{2}=\mathrm{v}_{0}{ }^{2}+2 \overrightarrow{\mathrm{a}} \cdot \overrightarrow{\mathrm{s}}v2=v02+2a⋅s
r→=r→0+v→0t+12a→t2\overrightarrow{\mathrm{r}}=\overrightarrow{\mathrm{r}}_{0}+\overrightarrow{\mathrm{v}}_{0} \mathrm{t}+\frac{1}{2} \overrightarrow{\mathrm{a}} \mathrm{t}^{2}r=r0+v0t+21at2
v2=v02+2a⃗⋅(r⃗0−r⃗)v^{2}=v_{0}^{2}+2 \vec{a} \cdot\left(\vec{r}_{0}-\vec{r}\right)v2=v02+2a⋅(r0−r)
