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www.damtp.cam.ac.uk/user/lauga/papers/73.pdf26 Jul 2013: m=0. (q m)!(α1,0ρ). m m!(q m)! ), (3.24). 12 S. Michelin and E. ... general solution takes the same form, see (3.24). By matching c̃p, C̃p and C̃0 up to O(ε3/2), the values of b̃0, ãp and ap can then bedetermined, and -
T h e o p e n – a ...
www.damtp.cam.ac.uk/user/lauga/papers/29.pdf26 Jul 2013: F (r ) = C1 Iλ(kr ) C2 Kλ(kr ), (24). ... Applying the condition that p̂ is finite at r = 0 to equation (24)eliminates Kλ as a solution for F. -
PHYSICS OF FLUIDS 18, 091701 �2006� Experimental investigations of ...
www.damtp.cam.ac.uk/user/lauga/papers/14.pdf26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11. -
Fluid Dynamics of Bacterial Turbulence Jörn Dunkel,1 Sebastian…
www.damtp.cam.ac.uk/user/gold/pdfs/bacterial_turbulence.pdf29 May 2013: Although very dif-ferent in size and composition, these systems are oftenjointly termed ‘‘active’’ fluids, for which there is now arange of continuum theories [12,14–24]. ... 2(d)] we observe the linear scaling z Exy=2,with 24 m being roughly -
Efficiency optimization and symmetry-breaking in a model of…
www.damtp.cam.ac.uk/user/lauga/papers/44.pdf26 Jul 2013: The first type of model, termed sublayer modeling, con-siders the dynamics of individual cilia, either theoretically ina simplified fashion,4,5 or numerically with all hydrodynamicinteractions.24,25 The study ... 1. Ln x0, t2. x0 tdx0. 24. For a given -
The friction of a mesh-like super-hydrophobic surfaceAnthony M. J. ...
www.damtp.cam.ac.uk/user/lauga/papers/33.pdf26 Jul 2013: 24–26 The second type of surface, less stud-ied, is one where the solid is the continuous phase, and theliquid/air contact occurs on isolated domains Fig. ... whose solution is. f xns, f yns =An, Bn. 1 s21/2 1 s 1 , 24. -
Orientational order in concentrated suspensions of…
www.damtp.cam.ac.uk/user/lauga/papers/61.pdf26 Jul 2013: Typicalvalues for b range from $%1 for bacteria like E. coli,6 $0for Volvox and artificially created squirmers17,24,27 to $þ1for Chlamydomonas.19. -
Membrane Viscosity Determined from Shear-Driven Flow in Giant…
www.damtp.cam.ac.uk/user/gold/pdfs/membrane_viscosity.pdf17 Jul 2013: second fluid withoutthe membrane [23,24]. ... 174, 381 (1987).[24] K.SugiyamaandM.Sbragaglia,J.Eng.Math.62,35(2008).[25] F. G. Woodhouse and R. E. Goldstein, J. -
Geometric transition in friction for flow over a bubble ...
www.damtp.cam.ac.uk/user/lauga/papers/25.pdf26 Jul 2013: We also plot in Fig. 3 the results ofour model for both surface coverage considered in the twoprevious studies: = 0.43 dashed line and = 0.68 solidline.24. -
Adhesion transition of flexible sheets Arthur A. Evans1,* and ...
www.damtp.cam.ac.uk/user/lauga/papers/27.pdf26 Jul 2013: minima in the free energy see Ref. 24 for a textbook treat-ment. ... Rev. E 76,. 061914 2007.24 M. Kardar, Statistical Physics of Fields Cambridge University.
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