Trying to derive the work equation in a conservative field after a few years of zero practice had me stump for an hour with simple derivatives.
I know that: $\mathrm d(\vec{v} \cdot \vec{v}) = (\mathrm d\vec{v})\cdot\vec{v} + \vec{v}\cdot(\mathrm d\vec{v}) = 2 (\vec{v}\cdot\mathrm d\vec{v})$
How do I show that: $\vec{v}\cdot\mathrm d(m\vec{v}) = \frac{m}{2}\mathrm d(\vec{v}\cdot \vec{v})$?
In this case, $m$ is a constant value.
This is in reference to Derivation in the link kinetic_energy