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8 Jul 2009: ratio N/f, whose value at top left is 100 (5 200 km/2 km).

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.

10 Jul 2009: 200 F. Charru and E. J. Hinch. 100. 10–1. 10–1 100 101.

3 Sep 2009: Taking 201 200 grid points in the finitedomain, the discretized nonlinear equations are solved in po-lar coordinates on the rectangular grid by a Newton-Raphsoniteration procedure using a banded matrix

13 Jun 2009: In this case, N > 200 before the values (1.15) begin to offer an advantage (for the values(1.16) the scenario is much worse).

31 Jul 2009: July. 24,. 200. 9 w. ww. sci. ence. mag. org. Dow. ... coverslips coated with a 200 μm thick layer of Polydimethylsiloxane (PDMS) (Sylgard 184,Dow Corning Ltd, Coventry, UK) and sealed from outside with additional PDMS to create a.

15 Oct 2009: Effective dynamics for solitons in the nonlinear Klein Gordon. Maxwell system and the Lorentz force law. Eamonn Longand David Stuart†. Centre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OWA, England. dmas2@cam.ac.uk. Abstract. We

13 Jul 2009: Typically N was taken to be 100, but some simulations have also been performed with N = 50, 200, 400 and 800. ... W,, = 0.2, 11 realisations); A, N = 200 (W, = 0.4, three realisations); V, N = 400 ( W, = 0.4, five realisations); 0, N = 800 ( W’, = 0.4,

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.

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