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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: