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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.

19 Oct 2013: and has had over 200 individuals directly contribute code to the kernel.

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.

16 Oct 2013: Notes for NSTMathematical Methods III†. Recommended books:. H.F. Jones, Groups, Representations and Physics, 2nd edn. (Inst. of Physics,1998) [Excellent for this course, and beyond it to topics like SU(2) and SO(3).]. J. Mathews & R.L. Walker,

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).

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 Oct 2013: 1993; Camalet, Julicher & Prost 1999), the typicalperiod T 0.04 s (Brokaw 1965), and the drag coefficient ξ 0.003 Pa s in water(assuming an aspect ratio Λ/a = 200,

24 Jun 2013: An over-night culture was diluted 200 and grown for 5 h until theend of exponential growth when the proportion of motilecells is maximal [34].

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