Active particles confined to a spherical viscous interface undergo a finite-wavelength instability whose selected mode arises from the competition between vesicle radius and Saffman-Delbrück length, confirmed by linear analysis and nonlinear simulations using spin-weighted spherical harmonics.
& R/a.pc/m.pc/a.pc/s.pc/w.pc/a.pc/m.pc/y.pc , S.2002 Hydrodynamic fluctuations and instabilities in ordered suspensions of self-propelled particles
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Collective dynamics of active suspensions on curved viscous interfaces
Active particles confined to a spherical viscous interface undergo a finite-wavelength instability whose selected mode arises from the competition between vesicle radius and Saffman-Delbrück length, confirmed by linear analysis and nonlinear simulations using spin-weighted spherical harmonics.