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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.

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: 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.

5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system.

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

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

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:

15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24].

27 Aug 2012: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.

2 Sep 2012: On the other hand, recent advances frommicron-scale magnetically actuated tails [24] to syntheticmolecular rotors [25] now allow fabrication of arrays ofactive tails that can stir up the fluid. ... 2007); Small 4, 111 (2008).[24] R. Dreyfus et al.,