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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.

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.

19 Sep 2009: 2. 3. t. y(t) 0 5 10 15 20 25. 2. ... 20,0)pr,0. Moreover. L[p1,0] = 0L[p2,0] = 3bp0,0p21,0L[p3,0] = 6bp0,0p1,0p2,0 bp31,0. We can easily work out the initial values.

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.

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

14 Jul 2009: E = π. 0. π/20. [L{Γ}ge(φ,θ; Γ). ]2sin θ dθ dφ. ... 20 L. C. Nitsche and E. J. Hinch. more vigorously than they are thrown back toward the centreline.

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

10 Jul 2009: a!, b!, c! Spatiotemporal diagrams obtained ford5 20 mm at asame density contrast At. ... Tube diameterd5 20 mm. The slope of the dashelines5 0.25 @see Eq.14!#.