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  2. 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.
  3. 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).
  4. 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.
  5. §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.
  6. 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
  7. 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.
  8. 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
  9. 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.
  10. 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
  11. 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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