Velocity-alignment entropy production ($\frac{d}{dt}\int f\log f=d\iint K\rho {\rho }_{\star }dxd{x}_{\star }$)

For the mean-field alignment equation in $d$ position and $d$ velocity coordinates, put $\rho =\int f{d}^{d}v$. Its force has velocity-space divergence $-d\int K{\rho }_{\star }{d}^d{x}_{\star }$. Consequently integration by parts gives the nonnegative derivative in the title, assuming suitable positivity, decay and integrability. The fine-grained Gibbs entropy decreases because these dynamics contract phase space; the interaction is dissipative.