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GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...
www.damtp.cam.ac.uk/user/mem/oldftp/rupert-ford-thesis93.pdf19 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 -
Efficiency optimization and symmetry-breaking in a model of…
www.damtp.cam.ac.uk/user/lauga/papers/44.pdf26 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 -
A Generalized Sampling Theorem for StableReconstructions in Arbitrary …
www.damtp.cam.ac.uk/research/afha/people/anders/Adcock_Hansen1.pdf5 Oct 2013: The well known NS-Sampling Theorem [24, 26, 29, 30, 34] states that if. -
AR235-FL37-11.Tex
www.damtp.cam.ac.uk/user/phh/papers/annrev.pdf19 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 -
Propulsion by passive filaments and active flagella near boundaries…
www.damtp.cam.ac.uk/user/lauga/papers/43.pdf26 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. -
Halloween I
www.damtp.cam.ac.uk/user/mem/papers/LHCE/halloween1.html19 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. -
Optimal feeding is optimal swimming for all Péclet numbers ...
www.damtp.cam.ac.uk/user/lauga/papers/59.pdf26 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. -
Dynamic mechanisms for apparent slip on hydrophobic surfaces Eric ...
www.damtp.cam.ac.uk/user/lauga/papers/7.pdf26 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. -
Jet propulsion without inertiaSaverio E. Spagnoliea� and Eric Laugab� …
www.damtp.cam.ac.uk/user/lauga/papers/41.pdf26 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 = -
A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenShadrin.pdf5 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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