v → = Δ X → Δ t {\displaystyle {\overrightarrow {v}}={\frac {\Delta {\overrightarrow {X}}}{\Delta t}}}
S = d Δ t {\displaystyle S={\frac {d}{\Delta t}}\,\!}
v ¯ = Δ X t o t a l Δ t t o t a l {\displaystyle {\overline {v}}={\frac {\Delta X_{total}}{\Delta t_{total}}}}
S ¯ = d t o t a l Δ t t o t a l {\displaystyle {\overline {S}}={\frac {d_{total}}{\Delta t_{total}}}}
a ¯ = Δ v → Δ t t o t a l {\displaystyle {\overline {a}}={\frac {\Delta {\overrightarrow {v}}}{\Delta t_{total}}}\,\!}
Δ X → = v → i n i t i a l + v → f i n a l 2 × t {\displaystyle \Delta {\overrightarrow {X}}={\frac {{\overrightarrow {v}}_{initial}+{\overrightarrow {v}}_{final}}{2}}\times t}