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26 Jul 2013: 072102-2 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012). ... 072102-5 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012).

18 Jan 2013: iv) Integrable Nolinear Elliptic PDEs. J. Lenells and A.S. Fokas, Boundary Value Problems for the Stationary Axisymmetric Einstein Equations: A Rotating Disk, Nonlinearity 24, 177-206 (2011). ... iii) Gravitometry. V. Michel and A.S. Fokas, A Unified

26 Jul 2013: PHYSICS OF FLUIDS 24, 051902 (2012). Self-propulsion in viscoelastic fluids: Pushers vs. ... Fluid. Mech. 24, 313–358 (1992).3 N. A. Hill and T. J.

28 Dec 2013: Natural Sciences Tripos, Part IA. Lent Term 2012. 24 lectures. Tuesday, Thursdays and Saturdays at 9 am, starting 19 January.

28 Dec 2013: Natural Sciences Tripos, Part IA. Lent Term 2014. 24 lectures. Tuesday, Thursdays and Saturdays at 9 am, starting 16 January.

26 Jul 2013: σ aux = 0, (23). uaux = 0. (24)Taking the inner product of Eq. ... d V. (30). 103102-9 Pak et al. Phys. Fluids 24, 103102 (2012).

5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps

9 Oct 2013: 3. 24 Oct 2013 – Equilibrium of a solid body IIIMoment of a force (torque).

26 Jul 2013: 24),simplifies to. F̂ 〈U2〉=. V0. 〈Σ[u1]〉 :ûdV. (26). 64001-p4. Life at high Deborah number. ... 24] Leal L. G., Annu. Rev. Fluid Mech., 12 (1980) 435.[25] Blake J.

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

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.

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

26 Jul 2013: Ishida et al.[21]. Tyrrell and Attard[22]. Tyrrell and Attard[23]. Steitz et al.[24]. ... These sizes are in agreement with the ex-perimental evidence of bubbles in Refs.[21–24], as summa-rized in Table I, although somewhat smaller.

26 Jul 2013: 4 6 1 1 13 24 1 1 21 40 1 15 6 1 3 14 28 3 1 22 42 1 16 12 3 1 15a 30 3 1 23 ... 43 2 37 12 1 1 15b 30 3 1 24 60 15 18 16 3 1 16 32 3 1 25 48 1 19 18 3 1 17 34 3

24 Jun 2013: 2Department of Physics, University of Arizona, Tucson, Arizona 85721, USA(Received 10 April 2013; published 24 June 2013). ... Stocker,Phys. Fluids 24, 091107 (2012). [28] W. R. DiLuzio, L. Turner, M.

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.

8 Oct 2013: Camalet and F. Jülicher, New J. Phys. 2, 24 (2000).[21] Chlamydomonas Resource Center at the University of. ... Malasarn,Plant J. 66, 770 (2011). [24] 5 mM HEPES, 40 mM KCl, 10 mM CaCl2, pH 7.2.[25] K.

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: on 24 November 2009rspa.royalsocietypublishing.orgDownloaded from. 108 O. S. Pak and E. ... s 1 ab s. s 11. )(e. s4y e2y)cos2x. (3.24). 4.

26 Jul 2013: 24" as! 1 iDe1"!̃3!1"! 1 iDe2"#̃̇3! 1". =12. De2 De11 2iDe1. ... 32# 3#3 8#De1De2 3#3De1De2+ 24#De1. 2 4"! 20 3#2 12De12 8De1De2.

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: 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: also include an induced electrophoreticcomponent,24 proportional to their zeta potential and thestreaming electric field. ... Up(z) ) Uhydro(z) Uelec(z) UkBT (24). Uhydro(z) ) [1 - O(ad)]UPD(z)ex (25).

26 Jul 2013: However, as expected, thecapillary attraction leads to an additional compressive load (theUk2 term in eqn (24)). ... 1999, 82, 1991.24 B. J. Reynwar, G. Illya, V. A. Harmandaris, M.

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: 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: 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.

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: Fluid Mech. 24, 313–358 (1992). 071904-16 Y. Man and E. Lauga Phys. ... Soft Matter 7, 8169–8181 (2011).24 L. Zhang, K. E. Peyer, and B.

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,.

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: 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.

11 Nov 2013: un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). NB uses 1 function evaluation per step – goodNB difficult to start or change step size t – badNB Stable t.

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.

26 Jul 2013: Typical two-dimensional (a) and three-dimensional (b),(c) cilium kinematics as observed forPleurobrachia [24] and Mytilus edulis [25], respectively.Sketch of the coordinates (d) and of the forces and momentsthat ... Kung, J. Cell Biol. 87, 33 (1980).[24]

12 Nov 2013: 22 4.000000302 3.015609e-07 0.5011010 1.0482393. 23 4.000000147 1.467238e-07 0.4865479 1.0479823. 24 4.000000064 6.370571e-08 0.4341880 1.0530215.

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.

26 Jul 2013: Received 20 March 2007; accepted 16 May 2007; published online 24 August 2007. ... 083104-2 Eric Lauga Phys. Fluids 19, 083104 2007. Downloaded 24 Aug 2007 to 128.54.43.238.

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.

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.

3 Oct 2013: As a last example, we point out thatparticles diffusiophoretically transported by a homogene-ous solute gradient [24] should also display a very similarpropagative dynamics, as they also induce a weak far ... 23] A. M. Menzel, Phys. Rev. E 85, 021912

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: or motion and we will thus not consider chemical swimmers21–24. or solid bodies powered by external fields.25. ... 24 G. Ruckner and R. Kapral, Phys. Rev. Lett., 2007, 98, 150603.25 S.

26 Jul 2013: c ðv2s=DRÞk2, as could havebeen anticipated from the single-swimmer problem [24].However, hydrodynamic interactions result in a renormal-ization of this single-swimmer effect. ... 24] J. R. Howse, R. A. L. Jones, A. J. Ryan, T.

26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

17 Dec 2013: δε = τλ‖. 〈Fy〉W 2tot. τ. 0δα H ( ḟ , f̈ , α, α̇, α̈) dt, (24). ... Rev. Lett. 93 186001. [24] Tabata O, Hirasawa H, Aoki S, Yoshida R and Kokufuta E2002 Ciliary motion actuator using self-oscillating gelSensors Actuators A 95 234–8.

26 Jul 2013: 24) is now triv-ial and the swimmer orientation remains constant. Sincethe flow is irrotational, no hydrodynamic torque (fromvorticity) is present to modify the orientations of the par-ticles. ... 23)and (24) and obtain. M =2μσπa3. M ′1 M′2 0. M

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: Typicalvalues for b range from $%1 for bacteria like E. coli,6 $0for Volvox and artificially created squirmers17,24,27 to $þ1for Chlamydomonas.19.

26 Jul 2013: Received 24 June 2003; accepted 11 February 2004; published online 1 July 2004! ... 24! Here we effectively demonstrate that these ideasalso apply as well to slowly varying flows.