2015/04/28 by Adriano Tiribocchi, Raphael Wittkowski, Davide Marenduzzo +1 · 1 citation
Physics and Astronomy · #cond-mat.soft #cond-mat.stat-mech #physics.bio-ph #physics.flu-dyn
paper · pdf · doi:10.1103/physrevlett.115.188302
published as Phys. Rev. Lett. 115, 188302 (2015) · 7 pages, 4 figures
arxiv created 2015/04/28 · arxiv updated 2015/11/18
We present a continuum theory of self-propelled particles, without alignment interactions, in a momentum-conserving solvent. To address phase separation we introduce a scalar concentration field ϕ with advective-diffusive dynamics. Activity creates a contribution Σij=-ζ((∂iϕ)(∂jϕ)-(∇ϕ)2δij/d) to the deviatoric stress, where ζ is odd under time reversal and d is the number of spatial dimensions; this causes an effective interfacial tension contribution that is negative for contractile swimmers. We predict that domain growth then ceases at a length scale where diffusive coarsening is balanced by active stretching of interfaces, and confirm this numerically. Thus the interplay of activity and hydrodynamics is highly nontrivial, even without alignment interactions.