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41 - 50 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. Generfc5.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_02.pdf
    13 May 2009: Van,cn(α, β, nz) =. 0(t α)a(t β)cenφ(t) dt, (4.23). withφ(t) = zt log(t α) log(t β) (4.24). ... Iserles (DAMTP, University of Cambridge). 24. References. [1] Milton Abramowitz and Irene A.
  3. Long slender drops in a simple shear flow

    www.damtp.cam.ac.uk/user/hinch/publications/JFM98_305.pdf
    23 Jul 2009: The differential equation can be integrated directly taking Po = 24 to produce an implicit expression for the shape. ... z = 0s-1 F 24( 1 - F2). which when substituted in the volume constraint yields.
  4. doi:10.1016/S0377-0257(97)00022-0

    www.damtp.cam.ac.uk/user/hinch/publications/JNNFM72_31.pdf
    10 Jul 2009: For A60,with an initial capillary pressure of 0.76 times the total elastic modulus, a pre-stretch of 3 anda finite extension of L1 = 24 (cf. ... The continuous curves are (a) for A40,L1 = 77 and P = 5; (b) for A60, L1 = 24 and P = 3; (c) for A80 L1 = 4.5
  5. 03pa0244

    www.damtp.cam.ac.uk/user/hinch/publications/PRSLA460_2975.pdf
    10 Jul 2009: π2/24, 24/π) (0.4112, 7.639), although the numerical results suggestthat the analysis of 4 requires β 1 101 rather than β 1. ... 24/(βT ) (lower), wherein the factor 2 has been included to translate the lines.
  6. Extrinsic1b.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_09.pdf
    1 Dec 2009: 3.24). The corresponding result is the following. Theorem 2 Let f(y) be constant, then we have θ0 = 0, θ1 = ̺ and. ... θs = (s 1)̺, s 2.Proof We shall use formula (3.24) and proceed along the lines of theproof of Theorem.
  7. doi:10.1016/j.jnnfm.2006.04.003

    www.damtp.cam.ac.uk/user/hinch/publications/JNNFM136_157.pdf
    8 Jul 2009: σtotn = 1Ca. κn, on ΓM(t). (24). Since there is no fixed boundary in this problem, the purely.Lagrangian approach is well adapted to it. ... Non-Newtonian Fluid Mech. 110 (2–3)(2003) 77–102. [24] R.F. Liang, M.R. Mackley, Rheological
  8. Rotation of small non-axisymmetric particles in a simple shear flow

    www.damtp.cam.ac.uk/user/hinch/publications/JFM92_591.pdf
    23 Jul 2009: 7 2 13.3 19.7 34.0 % / a , 1.33 1.64 2.13 2-55 3.63 4.24 5. ... Even for r = 30 a 24 Yo variation from axisymmetry produces a drift in 6 from &7r to approximately.
  9. Convergence acceleration of modified Fourier series in one or ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_11.pdf
    13 Jun 2009: The the extension to bivariate functions was developed, without analysis,in [24, 25, 27]. ... The bivariate version of this method wasoriginally developed, without analysis, in [24, 25, 27].
  10. PHYSICS OF FLUIDS 18, 041701 �2006� Laser-induced fluorescence…

    www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_18_041701.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.
  11. Raining into shallow water as a description of the collapse of a…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM554_259.pdf
    8 Jul 2009: 2 a1.02r30. In both geometries, the final slope at the front is much lower than the slope thatwould be given by an internal angle of friction δ = tan1(µ) = 24.

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