Use and setFor unit particle mass, is both the number density and the mass density in the number convention of c. A fixed reference scale inside the logarithm changes by a constant multiple of the conserved total mass, leaving its derivative unchanged.
Both prefactors in the source's part (d) need correction. Multiplication of the mean-field alignment equation by and integration by parts givesExchange and , use the symmetry of , and average the two expressions:The printed right-hand side omits . This corrected velocity-alignment energy dissipation agrees with the pair-counting calculation in a.
For velocity-alignment entropy production, let . The velocity-space divergence is . Assuming and sufficient decay, integration by parts yieldsThe printed formula omits the factor from the three velocity components. In spatial dimensions, that factor would be . Zeros of can be treated by a regularized entropy calculation when the required integrability holds.
A concrete smooth counterexample to both printed coefficients is and , where is a positive normalized Gaussian distribution. The total mass is one, the total momentum is zero, and initially. The kinetic energy derivative is , whereas the printed formula gives . The entropy functional derivative is , whereas the printed formula gives .
The signs describe cooling of relative velocities and contraction in phase space: increases, so the fine-grained Gibbs entropy decreases. These dissipative particle dynamics are not an isolated Hamiltonian system; there is no contradiction with Liouville's theorem or the Boltzmann equation's usual entropy increase. The microscopic mechanism removing kinetic energy is outside this alignment model.