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PHYSICS OF FLUIDS 17, 103102 �2005� Brownian motion near ...
www.damtp.cam.ac.uk/user/lauga/papers/11.pdf26 Jul 2013: 2. order OKn. Downloaded 24 Oct 2005 to 18.51.1.222. Redistribution subject to A. ... Kn O a3. h3. 38b. Downloaded 24 Oct 2005 to 18.51.1.222. -
rsif.royalsocietypublishing.org ResearchCite this article: Sareh S,…
www.damtp.cam.ac.uk/user/gold/pdfs/biomimetic_cilia.pdf3 Jan 2013: S-shaped actuation [24] and asoft three-link manipulator with visual feedback [25]. ... frame sequence number17 21 24 1 5 9 13. frame sequence number17 21 24. -
Hydrodynamic Fluctuations in Confined Particle-Laden Fluids Nicolas…
www.damtp.cam.ac.uk/user/lauga/papers/84.pdf3 Oct 2013: As a last example, we point out thatparticles diffusiophoretically transported by a homogene-ous solute gradient [24] should also display a very similarpropagative dynamics, as they also induce a weak far ... 23] A. M. Menzel, Phys. Rev. E 85, 021912 -
C0SM00953A 3060..3065
www.damtp.cam.ac.uk/user/lauga/papers/49.pdf26 Jul 2013: or motion and we will thus not consider chemical swimmers21–24. or solid bodies powered by external fields.25. ... 24 G. Ruckner and R. Kapral, Phys. Rev. Lett., 2007, 98, 150603.25 S. -
Hydrodynamics of Confined Active Fluids Tommaso Brotto,1…
www.damtp.cam.ac.uk/user/lauga/papers/75.pdf26 Jul 2013: c ðv2s=DRÞk2, as could havebeen anticipated from the single-swimmer problem [24].However, hydrodynamic interactions result in a renormal-ization of this single-swimmer effect. ... 24] J. R. Howse, R. A. L. Jones, A. J. Ryan, T. -
Bioinspiration & Biomimetics Bioinspir. Biomim. 9 (2014) 016001…
www.damtp.cam.ac.uk/user/lauga/papers/85.pdf17 Dec 2013: δε = τλ‖. 〈Fy〉W 2tot. τ. 0δα H ( ḟ , f̈ , α, α̇, α̈) dt, (24). ... Rev. Lett. 93 186001. [24] Tabata O, Hirasawa H, Aoki S, Yoshida R and Kokufuta E2002 Ciliary motion actuator using self-oscillating gelSensors Actuators A 95 234–8. -
PHYSICS OF FLUIDS 18, 091701 �2006� Experimental investigations of ...
www.damtp.cam.ac.uk/user/lauga/papers/14.pdf26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11. -
DOI 10.1140/epje/i2012-12068-y Regular Article Eur. Phys. J. E (2012) …
www.damtp.cam.ac.uk/user/lauga/papers/70.pdf26 Jul 2013: 24) is now triv-ial and the swimmer orientation remains constant. Sincethe flow is irrotational, no hydrodynamic torque (fromvorticity) is present to modify the orientations of the par-ticles. ... 23)and (24) and obtain. M =2μσπa3. M ′1 M′2 0. M -
Halloween I
www.damtp.cam.ac.uk/user/mem/papers/LHCE/halloween1.html19 Oct 2013: For example, when the TearDrop IP attack was first posted to the web, less than 24 hours passed before the Linux community had a working fix available for download. -
Digital Object Identifier (DOI) 10.1007/s00220-013-1729-7Commun.…
www.damtp.cam.ac.uk/user/md327/CDT13_file.pdf14 Aug 2013: Received: 24 April 2012 / Accepted: 20 November 2012Published online: 21 May 2013 – Springer-Verlag Berlin Heidelberg 2013. ... J. Math. Phys 18, 1449 (1977)24. Penrose, R.: Nonlinear gravitons and curved twistor theory.
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