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8 Jul 2009: r/r0. h(r, t)r0. 10 15 200 5. 1. 2. 3. 4. ... u(r, t). gr0. r/r0. 10 15 200 5. 0.5. 1.0. 1.5.

10 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

30 Nov 2009: stone. For example,|Ã200,200| = 6.3005, while|Ã250,250| = 1.2515. This process is faster when descending along diagonals andsomewhatslower along rows and columns ofA: thus,|Ã0,275| = 2.4706 ... andω = 100. n 100 200 400 1000A2n,2n 3.8002 5.8006

14 Jul 2009: The annular channel was made of Plexiglas, with mean radius R = 200 mm, widthR = 40 mm and height h = 16 mm (figure 4a). ... The maximum allowed amplitudeof the plate motion was U0/ω = 200 mm.

10 Jul 2009: a b 1 b 2. 1.5 0.101 0.2682.0 0.136 0.2193.0 0.167 0.1894.0 0.187 0.1945.0 0.200 0.202.

13 Jul 2009: III A. npically, for each particle concentration, 30 particles were chosen with trajectories longer than a dimensionless time of 200 (based on time scale a/V,). ... 3 G 200 8 aJ 1 0 0 m. 0 0 50 1 0 0 1 5 0 2 0 0.

10 Jul 2009: 0 50 100 150 200 250 300 350 400 450 500 2. ... 200. 0. 200. 400. 600. 800. 1000. / µ3/ 2s. /µ 7/ 2s.

10 Jul 2009: Finally, we let s = 0.2 (leaving a space of 0.6 for chainfluctuations) and q = 200 in Eq.

10 Jul 2009: c) Schematic view of the density-wave regime. Pressure variations along the pipe are monitored by four sensors located alongthe tube at vertical distances of 200, 450, 700 and 950 mm ... 200. Dz. (mm. ). Figure 2. Spatio-temporal images of the

31 Jul 2009: The thickness of the adsorbed layer of molecules on the solid surface was found t o be very small, approximately 200 A, suggesting t h a t the drag reduction cannot