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2 Sep 2012: Rev. Fluid Mech. 24,313 (1992). [2] A. Einstein, Ann. Phys. (Leipzig) 17, 549 (1905).[3] P.

2 Sep 2012: A macroscopic scale model of bacterialflagellar bundlingMunJu Kim, James C. Bird, Annemarie J. Van Parys, Kenneth S. Breuer, and Thomas R. Powers. Division of Engineering, Brown University, Box D, Providence, RI 02912. Edited by Howard C. Berg,

2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

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

17 Apr 2012: 21:. 22:. 23:. 24:. 25:. 26:. 27:. 28:. 29:. 30:. 31:.

2 Sep 2012: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... sions. Chem Phys 375:557–567.24. Batchelor GK (1970) The stress system in a suspension of force-free particles.

2 Sep 2012: 24,313 (1992). [2] W. F. Paxton et al., J. Am. Chem.

2 Sep 2012: Lipidmembranes do behave as two-dimensional f luids and can sup-port shear (24). ... Cole L, Orlovich DA, Ashford AE (1998) Fungal Genet Biol 24:86 –100.7.

2 Sep 2012: Rev. Fluid Mech. 24,. 313 (1992).[3] X.-L. Wu and A. Libchaber, Phys.

2 Sep 2012: reinhardtii). Similar confine-ment can also occur in biofilms and in cellular transport near freesurfaces (24, 25), as well as in thin, mucous layers over ciliatedepithelia, such as line the human ... Phys Rev Lett 105:188101. 24. Oliver JK, Willis BL

28 Feb 2012: On rapid computation of expansions in ultraspherical. polynomials. Maŕıa José CanteroDepartamento de Matemática Aplicada. Centro Politécnico Superior de IngenierosUniversidad de Zaragoza. Spain. Arieh IserlesDepartment of Applied

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