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21 - 30 of 167 search results for katalk:PC53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 167 match some words.

  1. Results that match 1 of 2 words

  2. Pumping by flapping in a viscoelastic fluid On Shun ...

    www.damtp.cam.ac.uk/user/lauga/papers/38.pdf
    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.

  3. PHYSICS OF FLUIDS 25, 061701 (2013) Spontaneous autophoretic motion…

    www.damtp.cam.ac.uk/user/lauga/papers/80.pdf
    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.

  4. No Job Name

    www.damtp.cam.ac.uk/user/lauga/papers/8.pdf
    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).

  5. Extensibility enables locomotion under isotropic drag On Shun Pak ...

    www.damtp.cam.ac.uk/user/lauga/papers/55.pdf
    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.

  6. C2SM27089G 1711..1720

    www.damtp.cam.ac.uk/user/lauga/papers/74.pdf
    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.

  7. PHYSICS OF FLUIDS 25, 031701 (2013) Fluid elasticity increases ...

    www.damtp.cam.ac.uk/user/lauga/papers/77.pdf
    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

  8. Continuous breakdown of Purcell’s scallop theorem with inertiaEric…

    www.damtp.cam.ac.uk/user/lauga/papers/17.pdf
    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.

  9. A smooth future?

    www.damtp.cam.ac.uk/user/lauga/papers/51.pdf
    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.

  10. PHYSICS OF FLUIDS 25, 071904 (2013) The wobbling-to-swimming…

    www.damtp.cam.ac.uk/user/lauga/papers/81.pdf
    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.

  11. Hydrodynamic friction of fakir-like superhydrophobic surfaces

    www.damtp.cam.ac.uk/user/lauga/papers/42.pdf
    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).

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