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2 Sep 2012: The latter point is more fully discussed by theRochester group (24, 40); one of the most important insightsemphasized by these researchers is that the capillary–muscle con-tact surface area is ... Cornish-Bowden,A. & Cardenas, M. L. (Plenum, New York),

25 Apr 2012: from [1],. ẍµ1(1 x2)ẋ vx = α1ẏ α2y ι(t). 24. Figure 4.1: Equation (4.1).

28 Feb 2012: 24. another generating function,. Ψ(t) =. n=0. φn(z)tn. =. [1. (2c 1)α z(αz)2 4α|c|2z.

3 Oct 2012: 60 74.605.082 1002.52 61.90 35.10 26.80 74.815.415 914.67 60.40 35.60 24.80 73.765.766 853.45 59.40

2 Sep 2012: equation and originally proposed to modelthe development of a breeding population [24]. ... 24. G.B. Arfken, H.J. Weber, Mathematical Methods for Physi-cists (Academic Press, San Diego, 1995).

2 Sep 2012: 24 and more complex numericalsimulations where these phenomena have been observed;see, e.g., Refs. ... Rev. Lett. 77, 1406 1996.37H. Daido, Physica D 91, 24 1996.38H.

28 Feb 2012: 24. n Z+. Given the quindiagonal structure of C, we have.

18 Oct 2012: R.; Jayaram, B.; Young,. M. A.; Beveridge, D. L.ReV. Comput. Chem.1997, 11, 317.(24) Kantor, Y.; Kardar, M.Phys.

2 Sep 2012: LabVIEW wasused to trigger the camera and control the LED light intensity time series.The temperature in the sample chamber was 24.5 0.5 C. ... Trends Cell Biol4:305–310. 24. Friedrich BM, Jülicher F (2007) Chemotaxis of sperm cells.

2 Aug 2012: Then, if wetake. g = (q>q)γ/2 (24). for an appropriate choice of γ, we have.

2 Sep 2012: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum

16 Jul 2012: 24 P. Bader, A. Iserles, K. Kropielnicka & P. Singh. of accuracy exhibited in Figs 4.3–4 is clearly in excess of O(ε7/2. ),

10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage.

2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [7] T. Vicsek, A.

3 Sep 2012: tracking code,24 or manually selected on each image using. ImageJ software,25 depending on the contrast. ... 23 E. Sackmann and R. F. Bruinsma, ChemPhysChem, 2002, 3,262–269. 24 J.

8 Mar 2012: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k.

2 Sep 2012: Julicher, New J. Phys., 2000, 2, 24.18 J. R. Blake and M. ... Rev. Lett., 2009, 102, 168101.24 M. Polin, I. Tuval, K. Drescher, J.

2 Sep 2012: not new. In a prescient article, Finlayson & Scriven (24) argued that biological matter.

3 Oct 2012: Rev. Lett. 24, 156–159(1970). 8. G. M. Gibson, J. Leach, S. ... We use the power spectral density method [24] within arecently suggested optimized calibration protocol [26, 27].

6 Jun 2012: ithou. t per. mis. sion. P.H.Haynes Part II Mathematical Biology Lent Term 2012 24.

27 Aug 2012: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.

2 Sep 2012: Plant, Cell and Environment. (2003). 26,. 1–15. 2003 Blackwell Publishing Ltd. 1. Blackwell Science, LtdOxford, UKPCEPlant, Cell and Environment0016-8025Blackwell Science Ltd 200226845Role of cytoplasmic streaming in symplastic transportW. F.

27 May 2012: carteri isachieved by cells at the bend points, which undergo adistinct transition in cell shape [20,22-24,26-29]. ... More-over, concerted movements of cells with respect to theCB system are crucial for the process of inversion in V.carteri

31 Oct 2012: 1603.24. Propagation of a front into an unstable ferromagnetic state. 1623.25.

2 Sep 2012: and, by equation (24) and the integral (21),. dO _f12. d z (0)= (27). ... terms in equation (23) and the oxygen consumption term in equation (24) are zero.

2 Sep 2012: T̂ = N̂. 24. The curvature is the rate of rotation of T̂ about B̂, and. ... Comparison of Eqs. 21–24 reveals that2 =1. 2 22 and 3 = , where is the angle between.

2 Sep 2012: NUTRIENT UPTAKE BY A SELF-PROPELLED STEADYSQUIRMER. by VANESA MAGAR†. (Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Silver Street, Cambridge CB3 9EW). TOMONOBU GOTO. (Department of Mechanical Engineering,

2 Sep 2012: Pi[Vr/(r, - a)]2 = 277a2D2/rl(r1 - a)4. (24)The volume involved is approximately 8irr 2(r, - a), so the total stirring power ex-pended in this region

2 Sep 2012: 2 3 ) pDV-D'@iF28@ = 0, (2.24). D(D = 0, x = - 1 , o. ( ... To see how these expansions proceed, we first note that (2.24) may be integrated, using (2.25), to dbtain 0 so CDdS(76Z2)/ -1 V d Z = 0.

2 Sep 2012: FL43CH26-Koch ARI 15 November 2010 14:32. Collective Hydrodynamics ofSwimming Microorganisms:Living FluidsDonald L. Koch1 and Ganesh Subramanian21 School of Chemical and Biomolecular Engineering, Cornell University, Ithaca,New York 14853; email:

3 Oct 2012: Chem. Phys. 81, 6320 1984. 24 E. Allahyarov, H. Lowen, and S.

21 Oct 2012: 2. ]. 24. More termsMatching: main body region. Main body=. c2n3.