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  2. minimal

    www.damtp.cam.ac.uk/user/gold/pdfs/minimal.pdf
    24 Apr 2013: models for active systems have beenproposed [2, 17–24], but most of them have yet to be tested against experiments [14, 25]. ... where. M =(. 2 A 00 0. ) (0|k|2 2|k|4 i λ0kxv0)I (24).
  3. Membrane Viscosity Determined from Shear-Driven Flow in Giant…

    www.damtp.cam.ac.uk/user/gold/pdfs/membrane_viscosity.pdf
    17 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.
  4. flm1100223a

    www.damtp.cam.ac.uk/user/lauga/papers/54.pdf
    26 Jul 2013: J. Fluid Mech. (2011), vol. 681, pp. 24–47. c Cambridge University Press 2011doi:10.1017/jfm.2011.223. ... 5.24). where b is some real constant and. I (ζ, Ca) =1.
  5. 26 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.
  6. Swimming in Circles: Motion of Bacteria near Solid Boundaries ...

    www.damtp.cam.ac.uk/user/lauga/papers/12.pdf
    26 Jul 2013: wall and crash into it. Furthermore, the authors proposed a. Submitted June 24, 2005, and accepted for publication September 28, 2005. ... xx Þ! ; (24). which is very similar to that given by the simple physical.
  7. 1B Methods 27 . 1B METHODS LECTURE NOTES Richard ...

    www.damtp.cam.ac.uk/user/examples/B8Lb.pdf
    4 Oct 2013: Xn(x) = Bn sinnπx. Lλn =. n2π2. L2. (24). Note that the first set eq. ... 24) the timeequation gives. Tn(t) = Cn exp(Dn2π2. L2t). The general solution for θ̂ (with odd initial condition θ̂(x, 0)) is thus.
  8. 26 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
  9. Adhesion transition of flexible sheets Arthur A. Evans1,* and ...

    www.damtp.cam.ac.uk/user/lauga/papers/27.pdf
    26 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.
  10. PII: S0142-727X(02)00163-7

    www.damtp.cam.ac.uk/user/lauga/papers/2.pdf
    26 Jul 2013: a). Re 29, onset of local absolute instability at x 1:24 (b) Re 47,onset of linear global instability, (c) Re 100, (d) Re 175, (e)Re 235, (f) Re
  11. Inevitability of a magnetic �eld in the Sun'sradiative interiorD. …

    www.damtp.cam.ac.uk/user/mem/oldftp/solar-nature.pdf
    19 Oct 2013: Mon.Not. R. ast. Soc., (submitted)24. Nesme-Ribes, E., Sokolo, D., Ribes, J.C. &
  12. doi:

    www.damtp.cam.ac.uk/user/lauga/papers/79.pdf
    26 Jul 2013: 9500 Gilman Drive, La Jolla CA 92093-0411, USA. (Received 11 January 2013; revised 13 March 2013; accepted 24 April 2013).
  13. Two-dimensional flagellar synchronization in viscoelastic fluids

    www.damtp.cam.ac.uk/user/lauga/papers/37.pdf
    26 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.
  14. 26 Jul 2013: 4. Experimental Section. Reagents and Solutions: Cupric sulfate pentahydrate, nickel(II) chloride hexahydrate, nickel(II) sulfamate tetrahydrate, gold (Oro-temp 24 RTU RACK) and silver (1025 RTU @ 4.5 Troy/gallon) ... HeLa cells were plated 24 h earlier
  15. flm1100081a

    www.damtp.cam.ac.uk/user/lauga/papers/50.pdf
    26 Jul 2013: 2000 Generic aspects of axonemal beating. New J. Phys. 2, 24.
  16. doi:

    www.damtp.cam.ac.uk/user/lauga/papers/73.pdf
    26 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
  17. §2 DYNAMICS §2.1 Surface vs. body forces, and the ...

    www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/dyn.pdf
    19 Oct 2013: 24. NB: Fluid initially at rest is an important special case.
  18. 1B Methods 1 . 1B METHODS LECTURE NOTES Richard ...

    www.damtp.cam.ac.uk/user/examples/B8La.pdf
    4 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.
  19. Optimal wavelet reconstructions from Fourier samples viageneralized…

    www.damtp.cam.ac.uk/research/afha/people/anders/samptaFinal.pdf
    5 Oct 2013: R. Driscoll, “Wavelet-encodedMR imaging,” Magn. Reson. Med., vol. 24, pp. 275–287, 1992.
  20. PHYSICAL REVIEW E 83, 011901 (2011) Locomotion by tangential ...

    www.damtp.cam.ac.uk/user/lauga/papers/46.pdf
    26 Jul 2013: Following classical modelingapproaches [22–24], the deviatoric stress τ can be splitedinto two components, the viscous solvent stress (τ s ) and thepolymeric stress (τ p); τ s is thus given by. ... 1: Fluid Mechanics 2nd ed. (WileyInterscience, New
  21. Proc. NATO Adv. Res. Workshop ARW 920946, Paris, October ...

    www.damtp.cam.ac.uk/user/mem/oldftp/qbosolar.pdf
    19 Oct 2013: variable between about 24 and 36 months — owe their existence and timing to the ir-. ... cycle taking, of course, about 24 to 36 months. The time-altitude contour plot of the.

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