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26 Jul 2013: 2. order OKn. Downloaded 24 Oct 2005 to 18.51.1.222. Redistribution subject to A. ... Kn O a3. h3. 38b. Downloaded 24 Oct 2005 to 18.51.1.222.

4 Nov 2013: J. Fluid Mech. (2013), vol. 719, pp. 551–586. c Cambridge University Press 2013 551doi:10.1017/jfm.2013.23. Convective shutdown in a porous medium athigh Rayleigh number. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1.

26 Jul 2013: have been investigated iRef. 24. P license or copyright, see http://pof.aip.org/pof/copyright.jsp.

26 Jul 2013: 24),simplifies to. F̂ 〈U2〉=. V0. 〈Σ[u1]〉 :ûdV. (26). 64001-p4. Life at high Deborah number. ... 24] Leal L. G., Annu. Rev. Fluid Mech., 12 (1980) 435.[25] Blake J.

26 Jul 2013: to the cre-ation of flagella bundles propelling the cells forward as theyswim, as well as the disruption of such bundles when thecells change their swimming direction.22–24. ... U =h̄. 2f x. s. 24. Noting that d / dt = U we therefore get an equation

26 Jul 2013: 2010).[19] S. Camalet and F. Jülicher, New J. Phys. 2, 24 (2000). ... Phys. 46, 13 (1997).[24] T. R. Powers, Rev. Mod. Phys. 82, 1607 (2010).[25] L.

19 Oct 2013: Fluid. Dyn. Res., 24, 375–404.Janssen, P. A. E. M. 1982 Quasilinear approximation for the spectrum of wind-generated.

26 Jul 2013: metrical model for dinoflagellates.24,25 A dinoflagellate can. FIG. 1. (Color online) (a) Notation for. ... Julicher, “Generic aspects of axonemal beating,” New J. Phys. 2, 24 (2000).11T.

19 Oct 2013: π. L. L2 D2. As (y′) dy′. (4.24). This expression can be cross-checked by evaluating the y-components of the sourceand sink recoil forces in (3.6) to ... 5.24). The direction of RV is not, of course, exactly parallel to ŷ, but rather makes anO( 2)

26 Jul 2013: One such model is con-sidered in the discussion FENE-P, and we obtain the sameresults see also 24. ... S. Suarez and X. B. Dai, Biol. Reprod. 46, 686 1992.24 E.