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10 Jul 2009: 0.1. Figure 6. The rebound velocity ẋn() divided by n5/6 (continuous curve) and by n3/4(broken curve) as a function of 1/n, for a line of 200 ... The results for four longlines, with N = 100, 200, 400 and 800, collapse onto a single curve.

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: A number of 200 particles was injected for eachexperiment to give good statistics. ... For each experiment withpackets of a given size, a total 200 particles were injectedover several packets.

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 Nov 2009: In the present experiments, the recording begins 200 safter the transit of the front and lasts for t = 200 s.

10 Nov 2009: 210-6. 0 200 400 600 800 1000 1200. w′VS. w′VS. adφdz. ... τ /tS. Laφ0. 0. 100. 200. 300. 400. 500. 0 200 400 600 800.

28 Sep 2009: We acknowledge the support of the EPSRC. APPENDIX: RESOLUTION STUDY. Figure 19 shows the numerical results obtained withthree different grid sizes 50 50, 100 100, and 200 200, respectively with the ... We are therefore confident that the 100 100 gridused

8 Jul 2009: The field of view is 600 mm long and its lowerboundary is located at 200 mm above the gate valve thisregion of interest is initially saturated only with the heavytransparent solution. ... R. Soc.London, Ser. A 200, 375 1950. 5E. E. Zukoski, “The

10 Jul 2009: 8 confirm thscaling law in the convective-diffusive regime withC. 200. Eliminatingl between Eqs.9! ... 200–207. 2G. K. Batchelor and J. M. Nitsche, ‘‘Instability of stationary unbound.

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