L→=r→×P→\overrightarrow{\mathrm{L}}=\overrightarrow{\mathrm{r}} \times \overrightarrow{\mathrm{P}}L=r×P
τ⃗=r→×F→\vec{\tau}=\overrightarrow{\mathrm{r}} \times \overrightarrow{\mathrm{F}}τ=r×F
L→=dτ⃗dt\overrightarrow{\mathrm{L}}=\frac{\mathrm{d} \vec{\tau}}{\mathrm{dt}}L=dtdτ
F→=dP→dt\overrightarrow{\mathrm{F}}=\frac{\mathrm{d} \overrightarrow{\mathrm{P}}}{\mathrm{dt}}F=dtdP