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.
Articles by others on the same topic
There are currently no matching articles.