Particle of mass $m$ is moving on a straight line under the influence of a force generated by a potential and friction with the equation of motion: $$m \frac{d^2x}{dt^2}+2 \gamma \frac{dx}{dt} = -V'(x) $$
They say $\displaystyle \frac{d}{dt}E = \frac{d}{dt} \bigg[\frac{m}{2}\left(\frac{dx}{dt}\right)^2+V(x)\bigg] \color{blue}= -2\gamma \left(\frac{dx}{dt}\right)^2 \le 0$ so $E$ is monotically increasing.
Could someone please explain the second/blue equality? Thanks.
Multiplying the movement equation by $\dot x$ we have
$$ \frac{d}{dt}\left(\frac 12 m\dot x^2 + V(x)\right) = -\gamma \dot x ^2 $$
but
$$ E = \frac 12 m\dot x^2 + V(x) \;\;\mbox{the so called mechanical energy} $$
hence
$$ \frac{d}{dt}E = -\gamma \dot x ^2 \le 0 $$
the mechanical energy decays according to the work realized by the dissipative forces.