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2 Sep 2012: Received 5 July 2003; revised manuscript received 20 January 2004; published 4 June 2004). ... Each flagellum consists of arotary motor; a universal joint about 50 nm long, known asthe hook, and a helical filament 20 nm in diameter and about10 mm long.

12 Sep 2012: The dispersion medium may be a simple liquid or acomplex fluid itself (a polymer solution for instance) [20].The packing density is approaching the jamming situa-tion. ... J. E 15, 97 (2004).20. H. Van Damme, S. Mansoutre, P.

20 Oct 2012: 11. 10 20 30 40 50. 10-14. 10-11. 10-8. 10-5. 0.0120 40 60 80 100. ... 10-14. 10-11. 10-8. 10-5. 0.01. 20 40 60 80 100. 10-10.

27 Aug 2012: Putting y. (18). equation (16) gives. or. (20). (21). This represents a progressive wave of bending moment with a wavelength,velocity and direction of propagation similar to the wave of displacement;

2 Sep 2012: a5. 20. cossvtd. 1 L 24s4 2 6ad sinsvtd 1 O sL 4d ,ytorque. ... Schliwa, J. Cell Sci.109,509 (1996). [20] R. E. Goldstein and S.

28 Feb 2012: 0.552. 0.554. 0.556. 0 5 10 15 20 25 0. 1. ... 35–52. << /ASCII85EncodePages false /AllowTransparency false /AutoPositionEPSFiles true /AutoRotatePages /None /Binding /Left /CalGrayProfile (Dot Gain 20%) /CalRGBProfile (sRGB IEC61966-2.1)

2 Aug 2012: Wecan circumvent this problem if we consider instead the splitting. H̄(q, p, qt, pt) =. (1. 2p>p. )γ. (V (q) pt. )γ. (20). Separable Hamiltonian with kinetic energy quadratic in ... 20 Sergio Blanes, Arieh Iserles. 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.22.

25 Apr 2012: iσm)2pr2,m = 2(iσm)p′r1,m f(p0,0). (iσmpr1,m. )20. r. n=1. 1. n! In,r. ... iκm. [2p′2,m µ(p. 20,0 1)p2,m. ], m = 1, 2,. Thus.

2 Sep 2012: The 20 stock wasprepared by adding spores on sand to 10 ml of TB at roomtemperature in a Petri dish and allowing for 24 h of growth. ... Typical f luid velocities atthe free surface are in the range of 20 –200 ms, acceleratingas the meniscus slope

2 Sep 2012: 14. 15. 15. 16. 5 10 20 25. 0.2. 0.4. 0.0. ... J. Elfring and E. Lauga, Phys. Rev. Lett. 103, 088101. 2009.20 M.