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  1. Results that match 1 of 2 words

  2. Noise and Synchronization in Pairs of Beating Eukaryotic Flagella ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinPolinTuval09.pdf
    16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.
  3. VOLUME 80, NUMBER 4 P H Y S I ...

    www.damtp.cam.ac.uk/user/hinch/publications/PhysRevLett.80.704.pdf
    10 Jul 2009: For the same trial as in Fig. 5, this constantB is found to be20.90 and 24.29 for the large andsmall angle sides, respectively.
  4. Effective dynamics for solitons in the nonlinear Klein Gordon ...

    www.damtp.cam.ac.uk/user/dmas2/public_ps/dl_final.pdf
    15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details.
  5. http://journals.cambridge.org Downloaded: 31 Jul 2009 IP address:…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM66_1.pdf
    31 Jul 2009: SZAN-IAWSKI, A. 1972 Arch. Mech. 24, 555. TANNER, R. I. 1971 J.
  6. Buoyancy driven miscible front dynamics in tilted tubesT. Séon,a! ...

    www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_17_031702.pdf
    8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex, 05, France. ... Rev.Fluid Mech. 24, 21 s1992d. 12F. Viana, R. Pardo, R. Yanez, and J.
  7. Instability of a high-speed submerged elastic jet

    www.damtp.cam.ac.uk/user/hinch/publications/JFM288_311.pdf
    14 Jul 2009: 0.24 1. 0.18. (T 0.12. 0.06. 0 a. FIGURE 2. The growth rate 0 = aci as a function of wavenumber CI for the varicose mode of a ... The dashed curves are contours of pressure. 0.24. 0.18. 0 0.12.
  8. 98PA207

    www.damtp.cam.ac.uk/user/hinch/publications/PRSLA455_3201.pdf
    10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7.
  9. PII: 0377-0257(93)80029-B

    www.damtp.cam.ac.uk/user/hinch/publications/JNNFM50_161.pdf
    13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C.
  10. persescribeericalma- trulyinedwith CPUwith iodicpen-la-tua- ize of…

    www.damtp.cam.ac.uk/user/hinch/publications/JFG000957.pdf
    10 Jul 2009: 1 O f 11/3! (24). Figure 3 shows the settling velocity for a simple cubic arrayspherical particles as a function off 1/3. ... It can be seen that thenumerical results, obtained by considering the finite size ofparticles, yield close agreement with the
  11. Buoyant mixing of miscible fluids in tilted tubesT. Séon, ...

    www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_16_L103.pdf
    8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.

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