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  2. GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...

    www.damtp.cam.ac.uk/user/mem/oldftp/rupert-ford-thesis93.pdf
    19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret
  3. Efficiency optimization and symmetry-breaking in a model of…

    www.damtp.cam.ac.uk/user/lauga/papers/44.pdf
    26 Jul 2013: The first type of model, termed sublayer modeling, con-siders the dynamics of individual cilia, either theoretically ina simplified fashion,4,5 or numerically with all hydrodynamicinteractions.24,25 The study ... 1. Ln x0, t2. x0 tdx0. 24. For a given
  4. A Generalized Sampling Theorem for StableReconstructions in Arbitrary …

    www.damtp.cam.ac.uk/research/afha/people/anders/Adcock_Hansen1.pdf
    5 Oct 2013: The well known NS-Sampling Theorem [24, 26, 29, 30, 34] states that if.
  5. AR235-FL37-11.Tex

    www.damtp.cam.ac.uk/user/phh/papers/annrev.pdf
    19 Oct 2013: 23 Nov 2004 1:27 AR AR235-FL37-11.tex AR235-FL37-11.sgm LaTeX2e(2002/01/18) P1: IBD10.1146/annurev.fluid.37.061903.175710. Annu. Rev. Fluid Mech. 2005. 37:263–93doi: 10.1146/annurev.fluid.37.061903.175710. Copyright c 2005 by Annual Reviews. All
  6. 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.
  7. Halloween I

    www.damtp.cam.ac.uk/user/mem/papers/LHCE/halloween1.html
    19 Oct 2013: For example, when the TearDrop IP attack was first posted to the web, less than 24 hours passed before the Linux community had a working fix available for download.
  8. Optimal feeding is optimal swimming for all Péclet numbers ...

    www.damtp.cam.ac.uk/user/lauga/papers/59.pdf
    26 Jul 2013: Thesecond mode (n2) defines the local stress applied by theswimmer on the surrounding fluid.8,24. ... cðr; lÞX1m0. CmðrÞLmðlÞ: (26). Substituting Eq. (26) into Eqs. (24) leads after projection on.
  9. 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.
  10. 26 Jul 2013: Other simple propulsivesystems proposed for locomotion at zero Reynolds numberinclude a deformable two-dimensional loop;18 systems oftwo,19–22 three,21,23,24 or N spheres;25 an oscillating body ... R2. z c. R1, 24. where c = a2 b2, r = x2 y2, r̂ =
  11. A stability barrier for reconstructions from Fourier samples Ben ...

    www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenShadrin.pdf
    5 Oct 2013: xm} is a grid of mequispaced points in [1, 1]. In [24] it was shown that. ... Proc. SPIE, 7535, 2010. [24] D. Coppersmith and T. Rivlin. The growth of polynomials bounded at equally spaced points.

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