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26 Jul 2013: 2. order OKn. Downloaded 24 Oct 2005 to 18.51.1.222. Redistribution subject to A. ... Kn O a3. h3. 38b. Downloaded 24 Oct 2005 to 18.51.1.222.

26 Jul 2013: 18 JULY 2008. 038102-2. wall-induced velocity is reminiscent of the shear-inducedmigration of deformable bodies and polymers away fromboundaries [21– 24], with the difference that, in thesecases, the dipoles ... Fluid Mech. 24,313 (1992). [20] J. R.

26 Jul 2013: 061701-2 Michelin, Lauga, and Bartolo Phys. Fluids 25, 061701 (2013). by interfacial stresses arising from the self-generated gradients of reactive surfactants.21, 24, 25 Unlikeautophoretic Janus particles, which swim ... Mater. 24, 811–816 (2012).7 P.

26 Jul 2013: F =1. 4. y02ISp. Sp4, 24. where ISp is a dimensionless integral defined by. ... 24, the measure-ments would show a decrease in the propulsive force nearboundaries.

20 May 2013: 2] Kapustin and Strassler, 9902033. 5. BZ la[ce spacing. 24 fermions! •

26 Jul 2013: Although suchcooperative effects have already been demonstrated forcoupled active but non-self-propelled particles in severaldifferent contexts 24–26, the generalization of our resultsto a large number of active particles remains ... Weinheim, Ger. 19,

26 Jul 2013: One such model is con-sidered in the discussion FENE-P, and we obtain the sameresults see also 24. ... S. Suarez and X. B. Dai, Biol. Reprod. 46, 686 1992.24 E.

26 Jul 2013: By scaling timesby 9. 5122f 24 / 21 and numbering the particles along the. ... 24 and 25 to ex-plicitly obtain at leading order in 1 / di j.

3 Jan 2013: S-shaped actuation [24] and asoft three-link manipulator with visual feedback [25]. ... frame sequence number17 21 24 1 5 9 13. frame sequence number17 21 24.

27 Feb 2013: Ann travels at a speed given. by β u/c = 24/25 in the x-direction for seven years and then comes back at the.

26 Jul 2013: without tail flexibilityno swimming can occur.5, 24 The second swimmer has a flat rubber tail (L = 20.5 mm, thickness t= 0.8 mm, width w = 3.4 mm, E = ... Rev. Lett. 80, 3879–3882 (1998).24 See supplementary material at

26 Jul 2013: 2010).[19] S. Camalet and F. Jülicher, New J. Phys. 2, 24 (2000). ... Phys. 46, 13 (1997).[24] T. R. Powers, Rev. Mod. Phys. 82, 1607 (2010).[25] L.

26 Jul 2013: J2k1/2(2πMa) cos 2kψ cos 2nψ (k 0). (2.24). Equation (2.24) is a symmetric infinite system of linear equations for the coefficients{cn; n 0}. ... The correspondingsolution of (2.24) is. c0 =4a. 3π. DL, cn = 0 (n > 0), (2.29).

26 Jul 2013: metrical model for dinoflagellates.24,25 A dinoflagellate can. FIG. 1. (Color online) (a) Notation for. ... Julicher, “Generic aspects of axonemal beating,” New J. Phys. 2, 24 (2000).11T.

26 Jul 2013: Langmuir 24, 12158–12163.BATCHELOR, G. K. 1972 Sedimentation in a dilute dispersion of spheres. ... Annu. Rev. Fluid Mech. 24, 313–358. PHONGIKAROON, S., HOFFMASTER, R., JUDD, K.

5 Oct 2013: J. Amer. Math. Soc., 24(1):81–124, 2011. 1.

26 Jul 2013: Here, the first effect of inertia is the appear-ance of a lift force directed across the undisturbedstreamlines.13,23,24 The original study, due to Saffman,23,24.

26 Jul 2013: be. L. L. a. V(z). Wetted. 0 s. 0 s. 24.5 s. ... Phys. Rev. Lett. 96, 186102 (2006).23. Squires, T. M. Phys. Fluids 20, 092105 (2008).24.

14 Aug 2013: Received: 24 April 2012 / Accepted: 20 November 2012Published online: 21 May 2013 – Springer-Verlag Berlin Heidelberg 2013. ... J. Math. Phys 18, 1449 (1977)24. Penrose, R.: Nonlinear gravitons and curved twistor theory.

26 Jul 2013: 9500 Gillman Drive, La Jolla California 92093-0411, USA(Received 15 January 2008; published 24 July 2008). ... J. Pedley and J. O. Kessler, Annu. Rev. Fluid Mech. 24,.