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Convergence acceleration of modified Fourier series in one or ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_11.pdf13 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]. -
VOLUME 80, NUMBER 4 P H Y S I ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysRevLett.80.704.pdf10 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. -
The effect of particle interactions on dynamic light scattering from…
www.damtp.cam.ac.uk/user/hinch/publications/JFM167_131.pdf23 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. -
Constitutive laws in liquid-fluidized beds
www.damtp.cam.ac.uk/user/hinch/publications/JFM452_371.pdf10 Jul 2009: J. Fluid Mech. (2002), vol. 452, pp. 371–404. c 2002 Cambridge University PressDOI: 10.1017/S0022112001007017 Printed in the United Kingdom. 371. Constitutive laws in liquid-fluidized beds. By P A U L D U R U 1, M A X I M E N I C O L A S1, J O H N -
PII: 0377-0257(93)80029-B
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM50_161.pdf13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C. -
Rotation of small non-axisymmetric particles in a simple shear flow
www.damtp.cam.ac.uk/user/hinch/publications/JFM92_591.pdf23 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. -
doi:10.1016/j.jnnfm.2003.10.001
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM116_141.pdf10 Jul 2009: C = 0.25χ′′u(0). ,µ. λ= 1.167, ν. λ= 3.00 (24). as |χ′′u(0)| , while for p = 2/3 and µs = 2 these coefficients are 0.24, ... 24) and (dash-dot) 13.0|C|3/2 from Eq. (21), with a numerical fit to thecoefficient. -
Generfc5.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_02.pdf13 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. -
Buoyant mixing of miscible fluids in tilted tubesT. Séon, ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_16_L103.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France. -
Extrinsic1b.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_09.pdf1 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.
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