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Model for dynamical coherence in thin films of self-propelled ...
www.damtp.cam.ac.uk/user/gold/pdfs/aranson07.pdf10 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. -
Microfluidics of cytoplasmic streaming and itsimplications for…
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_pnas.pdf10 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. -
PII: 0378-4371(89)90400-7
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/lekkerkerker.pdf10 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. -
doi: 10.1098/rsif.2011.0023, 1409-1417 first published online 2 March …
www.damtp.cam.ac.uk/user/gold/pdfs/plasticity_jrsi.pdf24 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. -
VOLUME 78, NUMBER 13 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/PRL78255597.pdf10 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. -
VOLUME 93, NUMBER 9 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/collective_prl.pdf10 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. -
VOLUME 87, NUMBER 6 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/reset.pdf10 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, -
VOLUME 80, NUMBER 23 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/PRL800523298.pdf10 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. -
Cosmological Einstein--Maxwell instantons and Euclidean supersymmetry
www.damtp.cam.ac.uk/user/md327/DGST1.pdf20 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. -
VOLUME 84, NUMBER 7 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/twirl.pdf10 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.
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