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  2. Adhesion induced non-planar and asynchronous flow of a giant ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/VezyMassieraViallat07.pdf
    3 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.
  3. Orthogonal polynomials on the unit circle and functional-differential …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_08.pdf
    28 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.
  4. No Job Name

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/nanopores/storm.pdf
    18 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.;
  5. Fluid Velocity Fluctuations in a Suspension of Swimming Protists ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/RushkinKantslerGoldstein10.pdf
    2 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.
  6. Generic Conditions for Hydrodynamic Synchronization Nariya Uchida1,*…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian11.pdf
    2 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.
  7. On expansions in orthogonal polynomials Maŕıa José…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_05.pdf
    28 Feb 2012: 20. normalise in his manner, rather than considering monic polynomials, since it makesfor somewhat simpler notation.
  8. PRL 95, 204501 (2005) P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HernandezOrtizStoltzGraham05.pdf
    2 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
  9. 201019079 10940..10945

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Drescheretal11.pdf
    2 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
  10. Synchronization and Collective Dynamics in a Carpet of Microfluidic…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian10.pdf
    2 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.
  11. The Mechanics and Statistics of Active Matter

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf
    2 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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