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5 Oct 2013: get. B =n. j=1. sp{χλ̃j (A)ξj,i}kji=kj11. sp{χλ̃n1 (A)ξn,i}Mi=kn1, n N 1,. 20.

3 Oct 2013: 730 R1-7. E. Lauga and C. Eloy. 102. 101. 103. 1005 10 150 20. ... 45. 40. 60. 35. 10. 0. –10. 20. –20. 0.50 1.0.

19 Oct 2013: 0.96. 40k. 1993. 20,000. 0.99. 100k. 1994. 100,000. 1.0. 170k. 1995.

5 Oct 2013: 0.5. 1. 1.5. 80 60 40 20 0 20 40 60 801. ... 0.5. 0. 0.5. 1. 1.5. 80 60 40 20 0 20 40 60 801.

19 Oct 2013: This factwill be used in (20) below. The flow in each of the two regions is expressed asan asymptotic expansion, with small expansion param-eter F. ... Solving(20) with decaying boundar y conditions as |X| ,we get. C 5 C K ( f R), (21)0 0 0iuC 5 C K ( f R

3 Oct 2013: Fluids 20,. 093303 (2008).[6] R. Di Leonardo, E. Cammarota, G. Bolognesi, H. ... 20] See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevLett.111.118301 for moredetails about the experiments and the data analysis.

26 Jul 2013: The time interval between each image is 20 ms. Scale bar 5 μm. ... M. Leshansky, Phys. Rev. E 2008, 77, 055305(R).[20] P. Tierno, O.

26 Jul 2013: microscopicconsiderations.20. ... Fluids 20(12), 123304 (2008). 24M. B. Short, C. A. Solari, S.

5 Oct 2013: 10. 20 40 60 80 1000. 0.5. 1. 1.5. 2. x 104. ... 20 10 0 10. 0.05. 0. 0.05. 10 5 0 5.

26 Jul 2013: p̂. r (20). Next, we need to express the no-penetration boundary condition at the wall in terms of p̂. ... Adv. Mater. 20 3453–6. New Journal of Physics 11 (2009) 075024 (http://www.njp.org/).

26 Jul 2013: In this case,the fluids involved (e.g. cervical mucus) have viscosities inthe range 0:1–10 Pa s [20], leading to values of ‘fbetween fractions of millimeters to meters. ... 20] D. P. Wolf, L. Blasco, M. A. Khan, and M.

19 Oct 2013: 1214 VOLUME 57J O U R N A L O F T H E A T M O S P H E R I C S C I E N C E S. q 2000 American Meteorological Society. Potential Vorticity Inversion on a Hemisphere. MICHAEL E. MCINTYRE AND WARWICK A. NORTON. Centre for Atmospheric Science, Department

19 Oct 2013: Sommeria,Myers, andSwinney,Nature 198986.4 cm dia.;rotation 20 rad/s (!). PV map anddye mapnear-identical. ... This is clearlya strong jet:staircase-like;eddy-transportbarrier. Sommeria,Myers, andSwinney,Nature 198986.4 cm dia.;rotation 20 rad/s (!). PV

19 Oct 2013: J.Phys. Oceanogr., 20, 1017–1042. Bleck, R., 1974: Short range prediction in isentropic coordinateswith filtered and unfiltered numerical models.

26 Jul 2013: Kenneth, Phys. Fluids, 2008, 20, 063104.67 A. M. Leshansky, O. Kenneth, O. ... du Roure, J. Marthelot, D. Bartolo and M. Fermigier,. Phys. Fluids, 2008, 20, 051703.79 B.

26 Jul 2013: shorter, such as the nodal cilia involved inembryonic development with L 2:5 m for mice [20]and L 5 m for humans [4], corresponding to Sp 1and Sp 2, respectively. ... J. Blum, Biophys. J. 41, 67 (1983).[20] J. H. E. Cartwright, O.

5 Oct 2013: showhow to construct the chart for f = id and refer to [6] [15] [20] for the general case. ... we can make a Hilbert manifold of Hs(M). The brief discussion above can be summarized inthe following theorem [20].

19 Oct 2013: 2 me p 1. 2.20. It is a limiting case in the sense that, if the absolutevorticity were lower (in absolute value) outside of pthan inside, the flow would be ... The two constraints (2.18) and (2.20) provide tworelationships for me:. 1 me 13.

26 Jul 2013: Low-Reynolds-number swimming in a capillary tube 297. –25. –20. –15. –10. ... 1.5. 0 20 40 60 80 100 120 140 160. –2–1.

26 Jul 2013: 32# 3#3 8#De1De2 3#3De1De2+ 24#De1. 2 4"! 20 3#2 12De12 8De1De2. ... 20 3#2 12De12 8De1De2. 3#2De1De2" sin 4"! 4 12De12 8De1De2". cos 2"!

26 Jul 2013: FIG. 7. Energy repartition of a cy-clonic unstable normal mode obtaineby the matrix eigenvalue method fok5 20 andk5 30. ... for k5 10 andk5 20 columns 2 and 3! Anextrapolated values 0 for k5 has been calculatedcolumn4!

26 Jul 2013: deal with the rotational Brownian motionof the swimmers,19 and to detail the microscopic coupling between the concentration gradients andthe fluid flows at small scales.20. ... Rev. Lett. 102, 188305 (2009).20 B. Sabass and U. Seifert, “Nonlinear,

19 Oct 2013: British Higher Education Policy in the last Twenty Years: The Murder of a Profession. Richard F. Gombrich. Tokyo, January 2000. Preamble. This is the text of a lecture I gave on 7 January 2000 in Tokyo at the Graduate Institute of Policy Studies

26 Jul 2013: σ ) xd V , (20). where we have assumed σ = 0 inside the solid body. ... Pedley, “Bioconvection,” Fluid Dyn. Res. 37, 1–20 (2005).4 J. W. Costerton, K.

26 Jul 2013: Received 31 July 2008; revised manuscript received 20 October 2008; published 3 December 2008. ... 18–20 and we see that. f1 1 2s/21 2 1/2. 48.

4 Nov 2013: The flow enters a new regime in which thebending stresses in (1) can be neglected almost every-where, resulting in a standard viscous gravity-currentbalance [7,20]. ... 19] L. Hocking, Q. J. Mech. Appl. Math. 36, 55 (1983).[20] H.

26 Jul 2013: 1, and for Re Ref, thefirst effect of inertia is the appearance of a lift force perpen-dicular to both the directions of translation and rotation13,19,20.

24 Jun 2013: At high concentrations, motile rodlike cells exhibit self-organization akin to nematic LC ordering [13,14,20], withthe added facet of polar alignment driven by collectiveswimming [21,22]. ... Properties of B. subtilis [31] and ofthe suspending medium

17 Dec 2013: Purcell’s three-link swimmer [17] was optimized[18–20], and so was a simpler version of the swimmer usingthree aligned spheres [21, 22]. ... 20)As f and α are both time-periodic function, we can use anintegration by part to obtain.

4 Oct 2013: 20). i.e. the energy is obtained by adding together contributions from separate sinusoidalharmonics whose energies are proportional to their squared amplitudes. ... If wesubstitute eq. (8) into Parseval’s formula eq. (20) we get L.

5 Oct 2013: get. B =n. j=1. sp{χλ̃j (A)ξj,i}kji=kj11. sp{χλ̃n1 (A)ξn,i}Mi=kn1, n N 1,. 20.

26 Jul 2013: dropping by about three orders of magnitudeto a value of approximately 20 times that of water. ... g1 =5. 144. 1. h ̄̄ ̄̄. 20. Finally, we find the first-order correction to the mechanicalenergy.

19 Oct 2013: a parabola) i.e., X = 12tY 2 (x0 12ty. 20 ). 4. The light dotted curves (below) show the cases t = 2, y0 = 0, x0 = 3.75, 3.5,. , ... 20 13y. 30 ). (Several lines of calculation — check it!) For x0 = 0 this is the solid curve in the plot below.It traces

4 Nov 2013: Comparingtheir figure 3 and (2.20) with our figure 2 and (2.11) highlights the importance ofthe specific system to the current behaviour. ... 10 cm above the porous medium within a large cylinder ofradius rC = 5.75 cm as it drained through the straws of

5 Oct 2013: 10. [6] R. Frank and C. Ueberhuber, Iterated Deferred Correction for Differential Equations,part 1, Computing, 20 (1978), 207-228. ... Comput. Phys., 189, 351–376, 2003. [15] B. Lindberg, Error Estimation and Iterative Improvement for Discretization

26 Jul 2013: Saintillan, M. Shelley, Phys. Fluids 20, 123304 (2008).11. D. Dendukuri, P.S. ... D. Saintillan, M.J. Shelley, Phys. Rev. Lett. 100, 178103(2008). 20. G.K.

26 Jul 2013: f iactt = 0 , 19. f iactt f j. actt = f 2t ti j , 20. ... Ishikawa, G. Sekiya, Y. Imai, and T. Yamaguchi, Biophys. J. 93, 2217 2007.20 G.

26 Jul 2013: s 1sin2x ab s. s 1 1sinx sin(x φ). a2 cos2(x φ)], (3.20). ... 1.0. 0.8. 0.6. 0.4. 0.2. 0 20. 10–20. 0.2. 0.4. 0.6.

26 Jul 2013: 3, 1701 2003.6 B. Bhushan, J. Phys.: Condens. Matter 20, 365214 2008.7 N. ... Oyharcabal and T. Frisch, Phys. Rev. E 71, 036611 2005.20 G.-W.

26 Jul 2013: 0 1 1 32. 1 3/20. 32. 3/2. 1 5/20 1. ... 0 1 1. 1 1/20. 1/2. 1 3/20 1. 1 2.

3 Feb 2013: Scale bar: 20 μm.) (B) The mutant pusher mbo1 remains trapped for several seconds (Movie S6). ... 20. Rüffer U, Nultsch W (1991) Flagellar photoresponses of Chlamydomonas cells heldby micropipettes: II.

17 Jul 2013: Because of its potential role in transport[18] there is great interest in the three-dimensionalcharacteristics of such shear-induced flows [19] and therole played by the intervening tonoplast [20]. ... E. Goldstein, J. Fluid Mech. 642, 5 (2010). [20] K.

26 Jul 2013: 0.5. 20.4. 271. 0.76. Bressac. etal.[17. ]Lygaeus. c[1]. [0.1]. [0.21]. [0.014]. ... 0.10. 0.15(a) (b). (c) (d). 0 20 40 60 80t t.

3 Jan 2013: t14 = 22.6 mst13 = 20.9 ms t15 = 24.3 ms t16 = 26.1 ms. ... The actuatorwas placed in the middle of a 50 50 20 cm3 tank filledwith deionized water.

4 Oct 2013: 0. 5. 10. 15. 20. Figure 1: Pn(x) for the top-hat, the Gaussian, and sin(nx)/(πx), showing convergencetowards the delta function, for n = 2, 4, 8, 16, 32 ... sin 1. 1x. f(ξ) sin(1 ξ)dξ. (20). Green’s functions for inhomogeneous BCs.

26 Jul 2013: A3y. x30, t = F0 cos t forced. 20. Here, M0 and F0 are the magnitudes of the time-varyingtorque and force, respectively. ... For human spermatozoa, the parameters areL 40 m and a 0.20 m.

4 Oct 2013: 20). 1B Methods 113. If we view the forcing term f(x,t) for each fixed time t = τ as an IC(!) at initial timet = τ then the integral in the ... 19). Then the time integral in eq. (20) expresses the forced solution θf asthe accumulation (superposition)

4 Nov 2013: In the inset offigure 2 (main text), this scatter is reduced by taking a 20-point running average.

26 Jul 2013: 98, 158102 (2007).[13] D. Saintillan and M. J. Shelley, Phys. Fluids 20, 123304 (2008). ... R. Trueman, The Locomotion of Soft-Bodied Animals (EdwardArnold, London, 1975). [20] M.

26 Jul 2013: These ve eigenfunctions become numerically indiscernible with double-precisionarithmetic when = 5:20 0:2. ... 5.1 0.9999 0.9999 0.9992 0.9988. 5.2 0.9999 0.9999 0.9999 0.9999. arithmetic when = 5:20 0:2.