Computer Simulation Study of Collective Phenomena in Dense by Timm Krüger PDF

By Timm Krüger

ISBN-10: 3834823759

ISBN-13: 9783834823755

ISBN-10: 3834823767

ISBN-13: 9783834823762

The rheology of dense pink blood phone suspensions is investigated through desktop simulations in response to the lattice Boltzmann, the immersed boundary, and the finite point equipment. The crimson blood cells are handled as prolonged and deformable debris immersed within the ambient fluid. within the first a part of the paintings, the numerical version and methods for pressure overview are mentioned. within the moment half, the habit of the suspensions in easy shear circulate is studied for various quantity fractions, particle deformabilities, and shear charges. Shear thinning habit is recovered. The lifestyles of a shear-induced transition from a tumbling to a tank-treading movement is tested. The transition will be parameterized by way of a unmarried volume, particularly the powerful capillary quantity. it's the ratio of the suspension rigidity and the attribute particle membrane tension. on the transition aspect, a powerful raise within the orientational order of the pink blood cells and an important reduce of the particle diffusivity are saw. even though, the typical mobilephone deformation indicates no signature of the transition.

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Extra info for Computer Simulation Study of Collective Phenomena in Dense Suspensions of Red Blood Cells under Shear

Example text

These relations have a certain freedom, which is the reason for the vast variety of different BC schemes for the LBM in the literature. One possible way to reconstruct the non-equilibrium populations is to employ eq. 21) or eq. 22) where the stress tensor may be found by extrapolation from the bulk region [127]. Another approach is to guess a stress tensor from the known, outgoing non-equilibrium populations as thoroughly discussed by Latt et al. [132]. It is also possible to employ the ‘bounce-back of non-equilibrium populations’ to reconstruct the missing populations [133].

Massless limit (mi → 0). Combining eq. 18) with eq. 16) directly results in the IBM force spreading equation, eq. 5), if the conservative force is identified as the membrane force. This finding also justifies that, in the present model, the elastic (conservative) membrane force is used in eq. 5) to drive the fluid (chap. 7). In the last step, keeping mi → 0, eq. 13), eq. 14), and eq. 18) are combined, which yields x˙ i = u(xi ) + 1 (F c + Fif ). 19) In the high friction limit (Γi → ∞), the no-slip condition is recovered and with it the IBM velocity interpolation, eq.

Initial conditions in the lattice Boltzmann method In many practical applications of hydrodynamics at small Reynolds numbers, the initial conditions do not play an important role. For steady flows, the flow field usually converges to the steady solution after some transient time, even if the initial conditions are not appropriately chosen. The reason is the viscous dissipation which erases the memory of the fluid. For unsteady flows at higher Reynolds numbers and, especially, for the study of transient effects, the initial conditions are relevant.

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Computer Simulation Study of Collective Phenomena in Dense Suspensions of Red Blood Cells under Shear by Timm Krüger


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