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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

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.

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.

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.

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

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.

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.

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

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: 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.