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Adhesion induced non-planar and asynchronous flow of a giant ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/VezyMassieraViallat07.pdf3 Sep 2012: propyltriethoxysilane and 5 mM acetic acid in water) for. 20 minutes under gentle mixing, rinsing with pure water,. ... Misbah, Phys. Rev. Lett., 83, 880–884.20 R. M. C. Dawson, D. -
Orthogonal polynomials on the unit circle and functional-differential …
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_08.pdf28 Feb 2012: p(12 ). 2. (ζ1). Let z = log(ζ)/(2i). Then. =. (1)q 12 (1)ζ = p1/4eizθ2(z,p),. 20. where θ2 is the second Jacobi theta function (Rainville 1960, p. -
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www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/nanopores/storm.pdf18 Oct 2012: Simulations of Manningcondensation on double-stranded DNA yield charge reductionvalues between 53% and 85%,22,23leading to a force estimateof 20-50 pN. ... E.; Perkins, T. P.; Chu, S.Macromolecules1996, 29, 1372.(20) Meller, A.; Nivon, L.; Brandin, E.; -
Fluid Velocity Fluctuations in a Suspension of Swimming Protists ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/RushkinKantslerGoldstein10.pdf2 Sep 2012: We consider themotion of colonies within a noninteracting ‘‘ideal gas’’model [20] which, despite its simplicity, gives satisfactoryagreement with the experiment; the fluid is unbounded, theswimmers are confined to a rectangular ... Drescher, K. -
Generic Conditions for Hydrodynamic Synchronization Nariya Uchida1,*…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian11.pdf2 Sep 2012: Thiscould be relevant to the synchronization of microswimmers[19], which can be minimally modeled by a linear configu-ration of three point forces [20]. ... 2009).[20] R. Golestanian and A. Ajdari, Phys. Rev. E 77, 036308. -
On expansions in orthogonal polynomials Maŕıa José…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_05.pdf28 Feb 2012: 20. normalise in his manner, rather than considering monic polynomials, since it makesfor somewhat simpler notation. -
PRL 95, 204501 (2005) P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HernandezOrtizStoltzGraham05.pdf2 Sep 2012: The fluid displayed intermittent flows in the. 05=95(20)=204501(4)$23.00 20450. form of swirls and occasionally jets, with length scales of10–20 m; this is of the ... Thefundamental mechanism behind this phenomenon is thatthe stresslet flow induced by -
201019079 10940..10945
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Drescheretal11.pdf2 Sep 2012: Edited by Jerry P. Gollub, Haverford College, Haverford, PA, and approved May 18, 2011 (received for review December 20, 2010). ... suspensions. Phys Fluids 20:123304.19. Baskaran A, Marchetti MC (2009) Statistical mechanics and hydrodynamics of bacterial -
Synchronization and Collective Dynamics in a Carpet of Microfluidic…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian10.pdf2 Sep 2012: 0. 0.2. 0.4. 0.6. 0.8. 1. 0 10 20 30 40 50 60 70 80 90. ... Netz, Phys. Rev. Lett. 96, 158101. (2006).[20] R. E. Goldstein, M. -
The Mechanics and Statistics of Active Matter
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf2 Sep 2012: obtained in the active-gel description (19, 20) of the cytoskeleton have precisely the same. ... cross-links, is also an active fluid suspension of polar orientable objects (8, 19, 20, 104,.
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