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Extensibility enables locomotion under isotropic drag On Shun Pak ...
www.damtp.cam.ac.uk/user/lauga/papers/55.pdf26 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. -
flm469.dvi
www.damtp.cam.ac.uk/user/lauga/papers/4.pdf26 Jul 2013: J. Fluid Mech. (2003), vol. 489, pp. 55–77. c 2003 Cambridge University PressDOI: 10.1017/S0022112003004695 Printed in the United Kingdom. 55. Effective slip in pressure-driven Stokes flow. By ERIC LAUGA AND HOWARD A. STONEDivision of Engineering -
C0SM00953A 3060..3065
www.damtp.cam.ac.uk/user/lauga/papers/49.pdf26 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. -
1B Methods 1 . 1B METHODS LECTURE NOTES Richard ...
www.damtp.cam.ac.uk/user/examples/B8La.pdf4 Oct 2013: u,Av) = (Bu,v) (24). (as you can easily check using the property that (Bu)† = u†B†). ... 36) of the µn values.). 1B Methods 24. 2.5 Parseval’s identity and least square approximations. -
atsc_56_2406.1236_1254
www.damtp.cam.ac.uk/user/mem/papers/SMINV/inv-ford-quasimanifold.pdf19 Oct 2013: 12 2 2 41 F f r 1 O(F lnF). 4(24). ... In particular, atO(1), this means that the coefficients of the lnr term in(18a) and (24) must agree, and hence. -
30 September 2012 Physics Today www.physicstoday.org In his long ...
www.damtp.cam.ac.uk/user/lauga/papers/71.pdf26 Jul 2013: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum -
doi:
www.damtp.cam.ac.uk/user/lauga/papers/79.pdf26 Jul 2013: 9500 Gilman Drive, La Jolla CA 92093-0411, USA. (Received 11 January 2013; revised 13 March 2013; accepted 24 April 2013). -
Two-dimensional flagellar synchronization in viscoelastic fluids
www.damtp.cam.ac.uk/user/lauga/papers/37.pdf26 Jul 2013: f2x =. 2π. 0. 〈τ2xy 〉|y=0 dx, (3.24). and only the mean component of the second-order stress, 〈τ2xy 〉, contributes tothe net force. -
PHYSICS OF FLUIDS 24, 103102 (2012) Micropropulsion and microrheology …
www.damtp.cam.ac.uk/user/lauga/papers/72.pdf26 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). -
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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