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  1. Results that match 1 of 2 words

  2. pnas201302736 14132..14137

    www.damtp.cam.ac.uk/user/gold/pdfs/streaming_selforganization.pdf
    27 Aug 2013: pointed) end to its plus (barbed) end.These cables are bound to the cortically fixed chloroplasts atthe cell periphery (24) in a “barber pole” twist, generating flowspeeds of 50–100 ... Characean algae. Proc Natl Acad Sci USA 73(1):165–167.24.
  3. Comparative Hydrodynamics of Bacterial Polymorphism Saverio E.…

    www.damtp.cam.ac.uk/user/lauga/papers/48.pdf
    26 Jul 2013: 2, 0.5) (1.1, 0.4)f (2.2, 0.53) (0.91, 0.29)g (2.3, 0.45) (0.69,1.52) (1.24, 0.52) (1.14,
  4. 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.
  5. Floppy swimming: Viscous locomotion of actuated elastica Eric…

    www.damtp.cam.ac.uk/user/lauga/papers/16.pdf
    26 Jul 2013: 0 aRFU 0 , 24. Text = 0 0 00 0 aRFU0 aRFU 0. ... Optimal III 0.24 3.34 12.6 2.6 7.9 0.336. Optimal IV 0.49 3.20 16.9 2.6 5.4 0.465.
  6. Confinement Stabilizes a Bacterial Suspension into a Spiral Vortex ...

    www.damtp.cam.ac.uk/user/gold/pdfs/confinement.pdf
    24 Jun 2013: 2Department of Physics, University of Arizona, Tucson, Arizona 85721, USA(Received 10 April 2013; published 24 June 2013). ... Stocker,Phys. Fluids 24, 091107 (2012). [28] W. R. DiLuzio, L. Turner, M.
  7. flm469.dvi

    www.damtp.cam.ac.uk/user/lauga/papers/4.pdf
    26 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
  8. 16 Oct 2013: m=1. α(m)(t)δmn. = α(n)(t) , (1.24). reproducing (1.23) apart from renaming the indices. ... 24. Chapter 2. 2. Groups. This chapter contains the second set of syllabus items, together with a fewitems anticipating the third set:.
  9. Asymptotic Solvers for Highly Oscillatory Semi-explicit DAEs Marissa…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_08.pdf
    12 Aug 2013: Cont. Dynamical Sys. 28, 1345–1367. 24. Figure 3.4: The errors for h(t) for ω = 200π (top row) and ω = 2000π(bottom row): from the left 0, 1 and
  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/people/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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