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26 Jul 2013: 440. D.L. egen. dre,. E.L. auga. and. J.M. agnaudet. Kn = 0 Re = 5 20 50 100 200 500 800. ... 1000.0. 0 0.5 1.0 1.5 2.0 2.5. 47.5. Kn. Re. Re = 200.

5 Oct 2013: 50 100 150 200. 10-10. 10-7. 10-4. 0.1 50 100 150 200. ... 10-14. 10-11. 10-8. 10-5. 0.01. 10. 50 100 150 200. 10-14.

26 Jul 2013: In 1963,Rothschild measured the distribution of bull spermatozoaswimming between two glass plates (separation 200 m).The cell distribution was nonuniform, with a constantdensity in the center strongly increasing near the ... 48:3 15 m; when H 200 m,

5 Oct 2013: m 25 50 100 200(i) 3.4e03 1.0e08 6.2e16 3.2e34(ii) 2.6e00 3.6e01 1.8e02 2.8e06(iii) 1.1e-03 2.9e-06 ... m 25 50 100 200 400(i) 4.1e00 3.5e00 3.5e00 3.3e00 3.3e00.

19 Jul 2013: ω2. )rather than O. (ω1. ). 11. Figure 3.2: |p0(t) y(t)| for ω = 12.5, 50, 200. ... Figure 3.3: |p0(t) p1(t,ω) y(t)| for ω = 12.5, 50, 200.

5 Oct 2013: 50 100 150 200. 10-10. 10-7. 10-4. 0.1 50 100 150 200. ... 10-14. 10-11. 10-8. 10-5. 0.01. 10. 50 100 150 200. 10-14.

26 Jul 2013: Re jjTxwjj2 jjTxwjj1 D2 D160 8.5 20.0 – –. H2 100 40.9 224.8 – –. 150 5541 17119 – –. 200 5,454,553 13,076,172 – –. 60 10.3 11.7 ... 150 6385 8594 þ15.2% 49.8%200 5,465,686 6,625,000 þ0.2% 49.3%. a H2 control and H1 control with the

3 Feb 2013: The second piece of history that I need to tell you about is from 200 years earlier. ... Newton’s theory had lasted more than 200 years. But Einstein was puzzled.

5 Oct 2013: m 25 50 100 200(i) 3.4e03 1.0e08 6.2e16 3.2e34(ii) 2.6e00 3.6e01 1.8e02 2.8e06(iii) 1.1e-03 2.9e-06 ... m 25 50 100 200 400(i) 4.1e00 3.5e00 3.5e00 3.3e00 3.3e00.

26 Jul 2013: 1 over 200 s. For these three cases (no swimming,steady swimming, and reciprocal swimming), we also plotas straight lines the theoretical prediction [where D isgiven, respectively, by DkBT, Eqs. ... 1 (averages of 500realizations over 200 s). Top to

26 Jul 2013: 3–200 s [Fig. ... h20. [17] Interestingly, for real spermatozoa, the swimming speedis only a fraction of the actuation speed of its flagel-lum (swimming at about 100–200 m=s with a30–60

26 Jul 2013: 200. 0 20 40 60 80 100. 0. 5x101. 1x102. 1.5x102. ... 200. 0 5x107 1x108 1.5x108 2x108. Mean. distan. ce. Mea. nd.

26 Jul 2013: difficult tosolve and double-precision arithmetic (the default precision in Matlab) becomesinadequate above Re 200.

4 Nov 2013: At the working distances typically used this resolution implies a spatialresolution of 5-7 pixels per millimetre (150 200 µm per pixel).

26 Jul 2013: System size R 250–800 µm 0.3–7 µm 6–12 mm 30 µm 40–200 nm. ... Slip length λeff 2–8 µm 20–90 nm 200–450 µm 1 µm 10–30 nm.

4 Nov 2013: Gravity and flow focusing in two-layered porous media 11. H0. 0 200 400 600 800. ... 100. 200. 300. 400. 0 20 40 60 80 100 120 140.

4 Nov 2013: 0 100 200 300t. (a) (b). FIGURE 5. (Colour online) The horizontally averaged solute flux F(t) (4.1), for a linearequation of state n = 1, aspect ratio L = 2 and ... 102. 101. 100. F. 100 200 300 400 5000 600t. FIGURE 7.

26 Jul 2013: line. The values of Gmaxare 10, 100, 200, 300, and 400 from the outer to the inner curve.

26 Jul 2013: the porous alumina membrane template containing 200 nm-diameter cylindrical pores (Catalog No 6809-6022; Whatman, Maidstone, UK) to serve as a working electrode. ... An open channel of 200 μm wide and 10 mm in length was used to properly visu-alize the

26 Jul 2013: 200. 400. 600. 800. 1000. 1200. 1400. φ3/π. -•o. φ2 = 0φ2 = π/6φ2 = π/2φ2 = 2π/3φ2 = 5π/6. ... 200. 400. 600. 800. 1000. 1200. 1400. FIG. 12. (Color online) Evolution of the rate of energy dissipationwith φ3 for different values of φ2.

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.

4 Nov 2013: efficiency of storage does indeed tend to a steady-state value. Six experiments wereconducted in a Hele-Shaw cell measuring 200 cm 30 cm 0.5 cm.

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.

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: 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.

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.

4 Nov 2013: Reservoir. 25 cm. Glycerineax. q. 200 cm. FIGURE 5. Schematic of the experimental Hele-Shaw cell. ... Colour online) Sequence of photographs showing the progression of experimentB at dimensional times (a) t = 20 s, (b) 100 s and (c) 200 s.

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.

26 Jul 2013: ForParamecium, the angular frequency is! 200 rad s1[1], and with the bending rigidity estimated to beB 25 pN m2 [19], one obtains Sp 4:6 in water.Some cilia are

26 Jul 2013: Two additional swimmers are also built. One had a rigid tail, made from of hypodermic tubing,(L = 25 mm, a = 125 µm, E = 200 GPa) and is used to demonstrate that

26 Jul 2013: Proc. R. Soc. Lond. A. 200, 523–541.Purcell, E. M. 1977 Life at low Reynolds number.

26 Jul 2013: 3 (a) Growth rate of the instability, s, as a function of wavenumber, k, for three values of the interaction strength, U, with external force F 200 (the value of thecritical ... For example, Fig. 3a shows the growth rate from eqn(24) as a function of

26 Jul 2013: Synchronization of flexible sheets 171. 100 200 300 400 500 600 700 8000.

26 Jul 2013: NaCl) using a rotary shaker (200 rpm) at 33C. Saturatedcultures were frozen at 70C in 15% glycerol. ... appropriate velocities and rotation rates are obtained if r isbetween 100 nm and 200 nm (46).

17 Jul 2013: with shearrate _. The chamber, typically 2 mm wide and 200 m deep,is made from polydimethylsiloxane by soft lithography andsealed with a glasscoverslipthat had been treated to promotevesicle adhesion.

5 Oct 2013: Generalized Sampling: Extension to Frames and Inverse andIll-Posed Problems. Ben Adcock Anders C. Hansen † Evelyn Herrholz ‡ Gerd Teschke‡. Abstract. Generalized sampling is new framework for sampling and reconstruction in