2007/09/30 by S. Kessler, S. KESSLER, R. Finken +3 · 2 citations
Materials Science · Medicine · Physics and Astronomy · #Block Copolymer Self-Assembly #Blood properties and coagulation #Computation #Deformation (meteorology) #Ellipsoid #Flow (mathematics) #Phase diagram #Polymer Surface Interaction Studies #Shear (geology) #Shear flow #Shear rate #Viscous liquid #cond-mat.soft
paper · pdf · doi:10.1017/s0022112008001493
published as Journal of Fluid Mechanics 605, 207-226 (2008) · 20 pages, 7 figures
openalex publication_date 2008/05/23 · arxiv created 2008/09/03 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The deformation of an elastic micro-capsule in an infinite shear flow is studied numerically using a spectral method. The shape of the capsule and the hydrodynamic flow field are expanded into smooth basis functions. Analytic expressions for the derivative of the basis functions permit the evaluation of elastic and hydrodynamic stresses and bending forces at specified grid points in the membrane. Compared to methods employing a triangulation scheme, this method has the advantage that the resulting capsule shapes are automatically smooth, and few modes are needed to describe the deformation accurately. Computations are performed for capsules with both spherical and ellipsoidal unstressed reference shape. Results for small deformations of initially spherical capsules coincide with analytic predictions. For initially ellipsoidal capsules, recent approximate theories predict stable oscillations of the tank-treading inclination angle, and a transition to tumbling at low shear rate. Both phenomena have also been observed experimentally. Using our numerical approach we can reproduce both the oscillations and the transition to tumbling. The full phase diagram for varying shear rate and viscosity ratio is explored. While the numerically obtained phase diagram qualitatively agrees with the theory, intermittent behaviour could not be observed within our simulation time. Our results suggest that initial tumbling motion is only transient in this region of the phase diagram.