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13 Jul 2009: a = 0.62 (stress Y -“.38) for 4 = 20. ... References. 1 R. Keunings, J. Non-Newtonian Fluid Mech., 20 (1986) 209-226.

17 Sep 2009: Penrose transform. In 1969, Penrose gave a formula for solutions to the wave equation inthe Minkowski space [20]:. ... Phys. 8 345–66[20] Penrose R 1969 Solutions of the zero-rest-mass equations J.

21 Jul 2009: This corresponds to particle Reynolds numbers in the range from 0.009 to 0.20, and the ratio of the sphere radius t o the pipe diameter a in the range

21 Jul 2009: 20, 111. ECKSTEIN, E. C. , BAILEY, D. G. & SHAPIRO, A.

21 Jul 2009: We may then put. m = (2 - 20)/(1- 20) where D = E(0)/2X,. ... King and D.F. James, J. Chem. Phys., 78 (1983) 4749-4754. 20 G.

10 Jul 2009: fluctuations and hydrodynamdiffusivity with the size of the numerical box,@14 –17,20#. ... For each case studied, dynamic simulations were made foto 20 realizations with different initial configurations.

15 Oct 2009: mN. )Φ1. ψ2r. 2rψ2 F1 = 0, (1.20). 2mψ2. Φ1r. F2 = 0, (1.21). ... the function u in (1.4)), and(eliminating ψ2 between (1.20)-(1.21)) the function Φ1 approaches ϕ, a solution of the Newton-Schrödingersystem (1.4).

8 Jul 2009: 5. Energy budgetThe initial potential energy in the tall column is E0 =. 12πgr20 h. 20 (axisymmetric) and. 12gr0h. 20 (planar). If one were to use the shallow-water equations to describe ... E/E0Eq/E0Dµ/E0Dq/E0(EiEq – Dµ – Dq)/E0. 15 20 25 300 5 10

24 Aug 2009: equation (14); ---- , equation (15); --- , equation (1 6 ). Calculated values from Brenner & Weiss- man ( 1 9 7 2 ) : 0, o / D = 20; 17, w / D = 40. ... It can be seen t h a t the numerical results for w / D = 20 and o / D = 40 are satisfactorily tending

8 Jul 2009: Experiments are performed in a longsL = 4 md perspextube of internal diameterd= 20 mm, with a sliding gate inthe middle, that can be tilted at anglesu from 0 to ... More quantitative results are obtained by recording witha digital camera images of the