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C1SM05503H 8169..8181
www.damtp.cam.ac.uk/user/lauga/papers/56.pdf26 Jul 2013: Flexible propeller10L 24 mm. Umax z 94 f 10 HzU z 22 mm s1a. ... The dimensionlessboundary conditions are. N(s 0) 0, (24). M(s 0) 0, (25). -
Optimal feeding is optimal swimming for all Péclet numbers ...
www.damtp.cam.ac.uk/user/lauga/papers/59.pdf26 Jul 2013: Thesecond mode (n2) defines the local stress applied by theswimmer on the surrounding fluid.8,24. ... cðr; lÞX1m0. CmðrÞLmðlÞ: (26). Substituting Eq. (26) into Eqs. (24) leads after projection on. -
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. -
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 -
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. -
Three-dimensional flows in slowly varying planar geometriesEric…
www.damtp.cam.ac.uk/user/lauga/papers/5.pdf26 Jul 2013: Received 24 June 2003; accepted 11 February 2004; published online 1 July 2004! ... 24! Here we effectively demonstrate that these ideasalso apply as well to slowly varying flows. -
Kinematics of the Most Efficient Cilium Christophe Eloy* and ...
www.damtp.cam.ac.uk/user/lauga/papers/68.pdf26 Jul 2013: Typical two-dimensional (a) and three-dimensional (b),(c) cilium kinematics as observed forPleurobrachia [24] and Mytilus edulis [25], respectively.Sketch of the coordinates (d) and of the forces and momentsthat ... Kung, J. Cell Biol. 87, 33 (1980).[24] -
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. -
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 -
flm1100223a
www.damtp.cam.ac.uk/user/lauga/papers/54.pdf26 Jul 2013: J. Fluid Mech. (2011), vol. 681, pp. 24–47. c Cambridge University Press 2011doi:10.1017/jfm.2011.223. ... 5.24). where b is some real constant and. I (ζ, Ca) =1. -
minimal
www.damtp.cam.ac.uk/user/gold/pdfs/minimal.pdf24 Apr 2013: models for active systems have beenproposed [2, 17–24], but most of them have yet to be tested against experiments [14, 25]. ... where. M =(. 2 A 00 0. ) (0|k|2 2|k|4 i λ0kxv0)I (24). -
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. -
British Higher Education Policy in the last Twenty Years: The Murder…
www.damtp.cam.ac.uk/user/mem/papers/LHCE/uk-higher-education.html19 Oct 2013: 24. The oldest strain of such non-conformism is Calvinist, Puritan. -
IB CATAM Project 0.1 (Preliminary Project)
www.damtp.cam.ac.uk/user/hinch/teaching/lectureHandout.pdf12 Nov 2013: 22 4.000000302 3.015609e-07 0.5011010 1.0482393. 23 4.000000147 1.467238e-07 0.4865479 1.0479823. 24 4.000000064 6.370571e-08 0.4341880 1.0530215. -
Crawling beneath the free surface: Water snail locomotionSungyon…
www.damtp.cam.ac.uk/user/lauga/papers/22.pdf26 Jul 2013: 24 represents aweak constraint on the validity of neglecting forces from theintermediate region. ... Furthermore, more systematicobservational studies are needed to identify which watersnail species exhibit which modes of “inverted crawling.” -
Swimming in Circles: Motion of Bacteria near Solid Boundaries ...
www.damtp.cam.ac.uk/user/lauga/papers/12.pdf26 Jul 2013: wall and crash into it. Furthermore, the authors proposed a. Submitted June 24, 2005, and accepted for publication September 28, 2005. ... xx Þ! ; (24). which is very similar to that given by the simple physical. -
Tuning gastropod locomotion: Modeling the influence of mucus…
www.damtp.cam.ac.uk/user/lauga/papers/15.pdf26 Jul 2013: h2. 2 ̄. 3 ̄ ̄̄. 24. III. RELEVANCE TO GASTROPOD CRAWLING:IMPACT OF RHEOLOGY ON LOCOMOTION COST. ... Zool. 24, 231984. 27M. W. Denny, “Invertebrate mucous secretions: Functional alternatives tovertebrate paradigms,” Symp. -
Time integration Issues ◮ Accuracy ◮ Cost◮ CPU = ...
www.damtp.cam.ac.uk/user/hinch/teaching/CMIFM_Handouts/TShandout.pdf11 Nov 2013: un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). NB uses 1 function evaluation per step – goodNB difficult to start or change step size t – badNB Stable t. -
1B Methods 27 . 1B METHODS LECTURE NOTES Richard ...
www.damtp.cam.ac.uk/user/examples/B8Lb.pdf4 Oct 2013: Xn(x) = Bn sinnπx. Lλn =. n2π2. L2. (24). Note that the first set eq. ... 24) the timeequation gives. Tn(t) = Cn exp(Dn2π2. L2t). The general solution for θ̂ (with odd initial condition θ̂(x, 0)) is thus. -
doi:
www.damtp.cam.ac.uk/user/lauga/papers/79.pdf26 Jul 2013: 9500 Gilman Drive, La Jolla CA 92093-0411, USA. (Received 11 January 2013; revised 13 March 2013; accepted 24 April 2013).
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