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20 Sep 2009: May form part of a larger settlement. • Requires 1,200 hectares or more. ... Norwich 14,100. • Broadland 12,200. • South Norfolk 11,200. • Ipswich 10,000. •

10 Jul 2009: on. July. 10,. 200. 9Pu. blis. hed. on J. anua. ry 1. ... 10,. 200. 9Pu. blis. hed. on J. anua. ry 1. 5, 1.

12 Nov 2009: R = 200 mm,h = 15 & 7 mm,η0 = 1 mm,λ = 50&70 mm,d = 0.5 mm,µ = 0.05 & 1 Pa s. ... L = 2 m, h = 11 & 16 mm, U0/ω 200 mm.

3 Sep 2009: 9. Fluid Dyn. Res. 41 (2009) 051403 N G Berloff. t=0 t=200. ... 12. Fluid Dyn. Res. 41 (2009) 051403 N G Berloff. t=0 t=200.

13 May 2009: This behaviour can be expected, since large values of. 23. 0 5 10 15 200. ... 5. 10. 15. 20. 25. 30. 35. 40. α. β. 0 5 10 15 200.

13 Jul 2009: It is interesting to note that at breakup a jet of a solution of 200 p.p.m. ... 51. They showed that several centimeter long strings of a 200 p.p.m.

8 Jun 2009: We. are therefore confident that the 100 100 grid used in this article is sufficiently accurate, whilecosting 116 th that of the 200 200 grid. ... Diameter (50x50)Diameter (100x100)Diameter (200x200). FIG. 19: Time evolution of droplet diameter using 50

30 Aug 2009: The atmosphere todaycontains about 200 Gton C in excess of the natural 1,750 value. ... time for the uptake would be determined by dividing 200 Gton C by 2 GtonC/year, to yield about 100 years.

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.

31 Jul 2009: http://journals.cambridge.org Downloaded: 31 Jul 2009 IP address: 131.111.16.227. 200 E. J. ... It is only after y / D = 200 that the viscosity as calculated from the exact.

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.

3 Sep 2009: nismsforcontinuouslyandcoherentlyrefillingtheBECsthesephe-nomena cannot be observed in atomic BECs. Losses are alwayspresent in BECs [200,201,13], and can even be induced throughthe use of focused electron beams [202].

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

21 Apr 2009: Figure 1: Absolute error |f (x, y) FN [f ](x, y)| for 1 x, y 1 (top row), 0.9 x, y 0.9 (bottom row) andN = 50, 100, 200. ... 200, for (x, y) = ( 34 ,23). (thickest line),(78,3.

24 Aug 2009: He calculated orientation-dependent angle averages for unrestricted aspect ratios, r , and values of y / D ranging from zero t o 200, where y is the shear rate. ... The latter value of 200 essentially represented the limitrs of storage capacity for the

10 Jul 2009: F 6. Time-lapse picture of the development of the interface at t 21.20, 21.57, 21.82, 22.00,22.12 and 22.20 with N 200 and γ ... J. Hinch. F 7. Time-lapse picture of the development of the interface at t 21.18, 21.53, 21.77,

13 Jul 2009: Non-Newtonian Fluid Mech., 44 (1992) 229-265 251. 6 I I I /. 5-. 4- PIPS. 1 ________.__.____________.-.----. No strand. 0 0 200 400 600 800 1000.

6 May 2009: Prandtl’s ratio N/f, whose value at top left is 100 (5 200 km/2 km).

26 May 2009: is even more important to achieve practical inexpensive results. We used stretchedgrids of size up to 200 200, in which the smallest and largest grid spacings differedby a factor of up

13 Jul 2009: o 1. lO 20 30 50. lOO 200 500 600 700 800.

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

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

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.

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).

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,

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

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

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.

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

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.

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.

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

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.

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: 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

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

5 Mar 2009: The annular channel was made of Plexiglas, with mean radius R = 200 mm, widthR = 40 mm and height h = 16 mm (figure 4a). ... R = 200 mm. U0 cos ωt. h. Figure 4. Sketch of the annular channel.

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