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1 - 10 of 79 search results for katalk:za33 24 |u:www.damtp.cam.ac.uk where 0 match all words and 79 match some words.

  1. Results that match 1 of 2 words

  2. 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.

  3. Existence and Newtonian limit of nonlinear bound states in ...

    www.damtp.cam.ac.uk/user/dmas2/public_ps/ed.pdf
    15 Oct 2009: 2ψ22) 2me2N Φ21. (e2N 1)2. 2me2Nψ22 4. rΦ1ψ2. = O(1),. (1.24). ... To see this, observe that by (1.24) and the preceding remarks, the equationF(l,Q,N, Φ1,ψ2; 0) = 0 amounts to.

  4. PublicationsDavid M.A. Stuart September 2009 1. Sophia Demoulini and…

    www.damtp.cam.ac.uk/user/dmas2/public_ps/publistcurrent.pdf
    28 Sep 2009: Equations, 30 (4), (2007), 523–546.24 pages. ... 24. D. Stuart, “Perturbation theory for kinks”, Communications in Mathematical Physics,149 (1992), 433-462.

  5. 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.

  6. Chlamy_science_full

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Polinetal09.pdf
    31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

  7. PII: 0169-7722(94)90073-6

    www.damtp.cam.ac.uk/user/hinch/publications/JCH16_87.pdf
    13 Jul 2009: ELSEVIER Journal of Contaminant Hydrology 16 (1994) 87-108. JOURNAL OF. Contaminant Hydrology. Echo tracer dispersion in model fractures with a rectangular geometry. I. I p p o l i t o a, G. D a c c o r d b, E.J. Hinch e, J.P. H u l i n a

  8. 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

  9. Heat transfer to a slowly moving fluid from a dilute fixed bed of…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM101_403.pdf
    23 Jul 2009: 4 ) gives in ( 3. 8 ) a contribution. 24 AT3 = $ K - = , q 5 ” 0 ( $ ) as # O , ( 3. ... 24 AT3 = = q5 - 89 O(q53ln q5) as q5 0.

  10. The effect of particle interactions on dynamic light scattering from…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM167_131.pdf
    23 Jul 2009: Rallison and E. J. Hinch. Without H I 1 84 1 1-24 - a9 With accurate HI 11.474 1-1.814 1-2.064 -2.224 Batchelor (1976, 1983) 1 ... pO as r / a c o , (3.24). and P-D;Vp = ikD,.P on r = 2a.

  11. Nonlinear drift interactions between fluctuating colloidal particles: …

    www.damtp.cam.ac.uk/user/hinch/publications/JFM256_343.pdf
    21 Jul 2009: 2.24). terms vanish for the mean. (2.25). (2.26). Relying on the decomposition (2.9) we now write the velocity field V as the sum of two contributions,. ... Ci = Ai Bi, (3.24). Here (O) denotes the semi-infinite fluid domain on one side, either right or

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