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8 Jun 2013: 200. 220. 240. 260. CO. 2 (p. p.m. v.). HoloceneYDB–AODLGM. –2,000 –1,500 –1,000 –500 0 500 1,000 1,500 2,000Lag (yr). ... METHODS SUMMARYThe data set compiled in this study contains most published high-resolution(median resolution, 200 yr),

26 Jul 2013: Although the surfaces usedwere nearly completely wetted by the solutions (contactangles close to zero), apparent slip lengths on the orderof λ 200 nm-1 µm were measured and were found todecrease ... If however |úp| ) 50 mV,we get λ 1 nm, and |úp| )

26 Jul 2013: 200 75 mm2 centered around the position x and normalized by thenumber of droplets in the same window for a close-packed crystal.

5 Oct 2013: We commence as follows:. 13. 10 20 30 40 50. 200.

19 Oct 2013: Such wavestravel at speeds just over 200 metres per second or 400 knots, not far short of the airspeeds of subsonicpassenger jet aircraft.).

26 Jul 2013: flow. Eukaryotic flagella and cilia have similar diameters ofthe order of 200 nm, beating frequencies of the order of 10Hz and internal structure. ... 24 to be computed accurately. Inthe representative cases presented in the rest of this work,typical

26 Jul 2013: G. Oldroyd, Proc. R. Soc. London, Ser. A 200, 523! 1950".#23$ R.

19 Oct 2013: Geophys. Astrophys.Fluid Dyn., 9, 185–200. Taylor, G. I. 1915 Eddy motion in the atmosphere.

5 Oct 2013: 18. 50 100 150 200 250 3000. 500. 1000. 1500. 50 100 150 200 250 3000. ... 19. 50 100 150 200 250 300 350. 0.9. 1.0. 1.1.

5 Oct 2013: 18. 50 100 150 200 250 3000. 500. 1000. 1500. 50 100 150 200 250 3000. ... 19. 50 100 150 200 250 300 350. 0.9. 1.0. 1.1.

19 Oct 2013: Solar tachocline dynamics: eddy viscosity,anti-friction, or something in between? MICHAEL E. McINTYRE. Centre for Atmospheric Science† at theDepartment of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce

19 Oct 2013: Geophys. Astrophys.Fluid Dyn., 9, 185–200. Taylor, G. I. 1915 Eddy motion in the atmosphere.

3 Jan 2013: Sens. Actuators A133, 200–209. (doi:10.1016/j.sna.2006.03.010). 20. Jung K, Nam J, Choi H.

24 Apr 2013: Quasi-stationary space–time averages 〈 〉 were computedover 3000 successive simulation time-steps (t = 0.1) after an initial relaxationperiod of 200 characteristic time units tu = L 4/γ2.

26 Jul 2013: Optimal feeding is optimal swimming for all Péclet numbers. Sébastien Michelin1,a) and Eric Lauga2,b)1LadHyX – Département de Mécanique, Ecole polytechnique, 91128 Palaiseau Cedex, France2Department of Mechanical and Aerospace Engineering,

26 Jul 2013: Propulsion in a viscoelastic fluidEric Laugaa. Department of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge,Massachusetts 02139, USA. Received 20 March 2007; accepted 16 May 2007; published online 24 August

26 Jul 2013: 1 – 104 s1 No-slip –. GlassOTS Glycerol 95 50 – 200 nm LWater 100 50 – 200 nm L.

26 Jul 2013: Floppy swimming: Viscous locomotion of actuated elastica. Eric LaugaDepartment of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA. Received 5 October 2006; published 26 April 2007.

26 Jul 2013: Both the Ni and Au. segments have a diameter of 200 nm.

7 Jan 2013: We determined the temperature-dependent distributions of θfrom more than 200 scattering events by tracking the position of thecell body up to a distance of 70 μm from the corner (Fig.