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10 Apr 2011: The last term in Eq. 1 describesthe coupling to strain rate tensor E Exy = xvy yvx 21,24.Our further analysis shows that while this term has somequantitative effect, e.g., ... F. Edwards, The Theory of Polymer DynamicsClarendon Press, Oxford, 1988. 24 N.

10 Apr 2011: 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.

10 Apr 2011: The electrostatic contribution was first determined by Odijk [24] and independently by Skolnick and Fixman [25] in the Debye- Hiickel approximation. ... 23). (24). H.N.W. Lekkerkerker I Curvature elasticity o f charged monolayers 325.

24 Aug 2011: on August 24, 2011rsif.royalsocietypublishing.orgDownloaded from. J. R. Soc. Interface (2011) 8, 1409–1417. ... 36 h. 12 h6 h 18 h. 24 h48/0 h. 42 h.

10 Apr 2011: Therefore, we expect the MSC to describe fronpropagation at smalla if it applies at all [24]. ... 23] H. Lamb, Hydrodynamics(Cambridge University Press,Cambridge, England, 1993), 6th ed. [24] Preliminary numerical studies by D.

10 Apr 2011: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P.

10 Apr 2011: This progression along the “devel-opmental path” [24] can work on a global scale to breakthe symmetry of circular waves, either by competition witha postulated third wave [19], tuning of the ... 24] A. Goldbeter and L. A. Segel, Differentiation 17,

10 Apr 2011: This and oobservations (e.g., of slow stress relaxation [24]) stronsuggest a dominant dissipative mechanismwithin the fila-ment, characterized by a very much largerzr. ... Chem. Phys.70, 2991. (1979); J. M. Schurr, Chem. Phys.84, 71 (1984).[24] J.

20 Jan 2011: American University ofBeirut, Beirut, Lebanon5 The Mathematical Institute, Oxford University, 24–29 St Giles, Oxford OX1 3LB, UK. ... Substituting (2.24) into (2.23) gives the system (2.18) for the1-forms ei.

10 Apr 2011: xj ij4s 1 Gas 2 1jsss. (10). Numerical solution [24] of (10) yields a critical valueac 8.9G [confirming dimensional analysis of Eq. ... Mod. Phys. 65, 851. (1993).[24] W. H. Press, W. T. Vetterling, S.

10 Apr 2011: 24 (SE = 0.03,P > 0.0001) and confirmed that section Volvox spe-cies have on average a significantly higher Vup thancolonies that do not retain robust cytoplasmaticbridges (estimate = 0.28,

11 Dec 2011: Prolongation II. k (Jk1(S2(TU))) (Jk(Pr(U))) (ker σk) obstructions0 9 4 5 01 18 12 6 02 30 24 6 03 45 40 5 04 63 60 3

10 Apr 2011: J Fluid Mech 647:201–219. 24. Călugăreanu G (1959) L’intégral de Gauss et l’analyse des noeuds tridimensionnels. ... Jordan arcs and prescribed surfaces. Proc Natl Acad Sci USA 24:97–101.33.

10 Apr 2011: 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.

10 Apr 2011: This canmodify significantly the rate of transport to an absorbing surface(24) and modify the hang time (25). ... 1976) Nature 259, 200 –201.24. Acrivos, A. & Taylor, T. D.

10 Apr 2011: 24, 321 (2002). [11] K. C. Leptos, J. S. Guasto, J.

10 Apr 2011: 4 A), representing either depletion or waste, alsoprovide spatially and temporally extended signals for the presenceof a colony, perhaps significant for intercolony communication, asin sexual induction (23) and quorum sensing (24), ... Michod, R. E. (2004

10 Apr 2011: Onemilliliter of 24-h stock was added to 50 ml of TB and incubated for18 h. ... O. (1992) Annu. Rev. Fluid Mech. 24, 313–358.12. Hillesdon, A. J., Pedley, T.

10 Apr 2011: 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.

10 Apr 2011: 2µR(µS. e. cAµ. ) Rµ. (µS. e. cAµ. )= 0 (24). ... ln R (i/η)S = ln to rewrite the pair of equations (24) and (25) as[(.