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PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: 4,5,24–30]. The individual locomotion of spermatozoa was first studiedby G. I. ... 24). The complete solution of the Stokes equations in cylindricalcoordinates to the first order in kb is therefore finally given by. -
Home Page of Prof. A.S. FOKAS
www.damtp.cam.ac.uk/user/tf227/18 Jan 2013: iv) Integrable Nolinear Elliptic PDEs. J. Lenells and A.S. Fokas, Boundary Value Problems for the Stationary Axisymmetric Einstein Equations: A Rotating Disk, Nonlinearity 24, 177-206 (2011). ... iii) Gravitometry. V. Michel and A.S. Fokas, A Unified -
PHYSICS OF FLUIDS 24, 072102 (2012) Buckling instability of ...
www.damtp.cam.ac.uk/user/lauga/papers/67.pdf26 Jul 2013: 072102-2 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012). ... 072102-5 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012). -
PHYSICS OF FLUIDS 24, 051902 (2012) Self-propulsion in viscoelastic…
www.damtp.cam.ac.uk/user/lauga/papers/66.pdf26 Jul 2013: PHYSICS OF FLUIDS 24, 051902 (2012). Self-propulsion in viscoelastic fluids: Pushers vs. ... Fluid. Mech. 24, 313–358 (1992).3 N. A. Hill and T. J. -
Mathematical Methods II
www.damtp.cam.ac.uk/user/gio10/nst1a_b.html28 Dec 2013: Natural Sciences Tripos, Part IA. Lent Term 2012. 24 lectures. Tuesday, Thursdays and Saturdays at 9 am, starting 19 January. -
Mathematical Methods II
www.damtp.cam.ac.uk/user/gio10/nst1a_a.html28 Dec 2013: Natural Sciences Tripos, Part IA. Lent Term 2014. 24 lectures. Tuesday, Thursdays and Saturdays at 9 am, starting 16 January. -
PHYSICS OF FLUIDS 24, 103102 (2012) Micropropulsion and microrheology …
www.damtp.cam.ac.uk/user/lauga/papers/72.pdf26 Jul 2013: σ aux = 0, (23). uaux = 0. (24)Taking the inner product of Eq. ... d V. (30). 103102-9 Pak et al. Phys. Fluids 24, 103102 (2012). -
www.damtp.cam.ac.uk/user/mem/oldftp/AIX/aixf.log
www.damtp.cam.ac.uk/user/mem/oldftp/AIX/aixf.log5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps -
Mechanics (non-examinable) Mathematical Tripos, Part IADr M B Wingate …
www.damtp.cam.ac.uk/user/wingate/Mechanics/schedule.pdf9 Oct 2013: 3. 24 Oct 2013 – Equilibrium of a solid body IIIMoment of a force (torque). -
June 2009 EPL, 86 (2009) 64001 www.epljournal.orgdoi:…
www.damtp.cam.ac.uk/user/lauga/papers/28.pdf26 Jul 2013: 24),simplifies to. F̂ 〈U2〉=. V0. 〈Σ[u1]〉 :ûdV. (26). 64001-p4. Life at high Deborah number. ... 24] Leal L. G., Annu. Rev. Fluid Mech., 12 (1980) 435.[25] Blake J. -
The real number line is a good model for ...
www.damtp.cam.ac.uk/user/tong/talks/numbers.pdf20 May 2013: 2] Kapustin and Strassler, 9902033. 5. BZ la[ce spacing. 24 fermions! • -
htl4.dvi
www.damtp.cam.ac.uk/user/tong/relativity/htl4.pdf27 Feb 2013: Ann travels at a speed given. by β u/c = 24/25 in the x-direction for seven years and then comes back at the. -
Dynamic mechanisms for apparent slip on hydrophobic surfaces Eric ...
www.damtp.cam.ac.uk/user/lauga/papers/7.pdf26 Jul 2013: Ishida et al.[21]. Tyrrell and Attard[22]. Tyrrell and Attard[23]. Steitz et al.[24]. ... These sizes are in agreement with the ex-perimental evidence of bubbles in Refs.[21–24], as summa-rized in Table I, although somewhat smaller. -
PRL 93, 238301 (2004) P H Y S I ...
www.damtp.cam.ac.uk/user/lauga/papers/9.pdf26 Jul 2013: 4 6 1 1 13 24 1 1 21 40 1 15 6 1 3 14 28 3 1 22 42 1 16 12 3 1 15a 30 3 1 23 ... 43 2 37 12 1 1 15b 30 3 1 24 60 15 18 16 3 1 16 32 3 1 25 48 1 19 18 3 1 17 34 3 -
Can everything be computed? - On the Solvability ComplexityIndex ...
www.damtp.cam.ac.uk/research/afha/projects/CCA_Project5_SCI.pdf5 Oct 2013: J. Amer. Math. Soc., 24(1):81–124, 2011. 1. -
Confinement Stabilizes a Bacterial Suspension into a Spiral Vortex ...
www.damtp.cam.ac.uk/user/gold/pdfs/confinement.pdf24 Jun 2013: 2Department of Physics, University of Arizona, Tucson, Arizona 85721, USA(Received 10 April 2013; published 24 June 2013). ... Stocker,Phys. Fluids 24, 091107 (2012). [28] W. R. DiLuzio, L. Turner, M. -
Hydrodynamic Attraction of Swimming Microorganisms by Surfaces…
www.damtp.cam.ac.uk/user/lauga/papers/20.pdf26 Jul 2013: 18 JULY 2008. 038102-2. wall-induced velocity is reminiscent of the shear-inducedmigration of deformable bodies and polymers away fromboundaries [21– 24], with the difference that, in thesecases, the dipoles ... Fluid Mech. 24,313 (1992). [20] J. R. -
Antiphase Synchronization in a Flagellar-Dominance Mutant of…
www.damtp.cam.ac.uk/user/gold/pdfs/antiphase.pdf8 Oct 2013: Camalet and F. Jülicher, New J. Phys. 2, 24 (2000).[21] Chlamydomonas Resource Center at the University of. ... Malasarn,Plant J. 66, 770 (2011). [24] 5 mM HEPES, 40 mM KCl, 10 mM CaCl2, pH 7.2.[25] K. -
Proc. R. Soc. A (2010) 466, 107–126doi:10.1098/rspa.2009.0208…
www.damtp.cam.ac.uk/user/lauga/papers/34.pdf26 Jul 2013: on 24 November 2009rspa.royalsocietypublishing.orgDownloaded from. 108 O. S. Pak and E. ... s 1 ab s. s 11. )(e. s4y e2y)cos2x. (3.24). 4. -
Pumping by flapping in a viscoelastic fluid On Shun ...
www.damtp.cam.ac.uk/user/lauga/papers/38.pdf26 Jul 2013: 24" as! 1 iDe1"!̃3!1"! 1 iDe2"#̃̇3! 1". =12. De2 De11 2iDe1. ... 32# 3#3 8#De1De2 3#3De1De2+ 24#De1. 2 4"! 20 3#2 12De12 8De1De2. -
No many-scallop theorem: Collective locomotion of reciprocal swimmers …
www.damtp.cam.ac.uk/user/lauga/papers/23.pdf26 Jul 2013: Although suchcooperative effects have already been demonstrated forcoupled active but non-self-propelled particles in severaldifferent contexts 24–26, the generalization of our resultsto a large number of active particles remains ... Weinheim, Ger. 19, -
PHYSICS OF FLUIDS 25, 061701 (2013) Spontaneous autophoretic motion…
www.damtp.cam.ac.uk/user/lauga/papers/80.pdf26 Jul 2013: 061701-2 Michelin, Lauga, and Bartolo Phys. Fluids 25, 061701 (2013). by interfacial stresses arising from the self-generated gradients of reactive surfactants.21, 24, 25 Unlikeautophoretic Janus particles, which swim ... Mater. 24, 811–816 (2012).7 P. -
No Job Name
www.damtp.cam.ac.uk/user/lauga/papers/8.pdf26 Jul 2013: also include an induced electrophoreticcomponent,24 proportional to their zeta potential and thestreaming electric field. ... Up(z) ) Uhydro(z) Uelec(z) UkBT (24). Uhydro(z) ) [1 - O(ad)]UPD(z)ex (25). -
Extensibility enables locomotion under isotropic drag On Shun Pak ...
www.damtp.cam.ac.uk/user/lauga/papers/55.pdf26 Jul 2013: metrical model for dinoflagellates.24,25 A dinoflagellate can. FIG. 1. (Color online) (a) Notation for. ... Julicher, “Generic aspects of axonemal beating,” New J. Phys. 2, 24 (2000).11T. -
C2SM27089G 1711..1720
www.damtp.cam.ac.uk/user/lauga/papers/74.pdf26 Jul 2013: However, as expected, thecapillary attraction leads to an additional compressive load (theUk2 term in eqn (24)). ... 1999, 82, 1991.24 B. J. Reynwar, G. Illya, V. A. Harmandaris, M. -
PHYSICS OF FLUIDS 25, 031701 (2013) Fluid elasticity increases ...
www.damtp.cam.ac.uk/user/lauga/papers/77.pdf26 Jul 2013: without tail flexibilityno swimming can occur.5, 24 The second swimmer has a flat rubber tail (L = 20.5 mm, thickness t= 0.8 mm, width w = 3.4 mm, E = ... Rev. Lett. 80, 3879–3882 (1998).24 See supplementary material at -
Continuous breakdown of Purcell’s scallop theorem with inertiaEric…
www.damtp.cam.ac.uk/user/lauga/papers/17.pdf26 Jul 2013: Here, the first effect of inertia is the appear-ance of a lift force directed across the undisturbedstreamlines.13,23,24 The original study, due to Saffman,23,24. -
PHYSICS OF FLUIDS 25, 071904 (2013) The wobbling-to-swimming…
www.damtp.cam.ac.uk/user/lauga/papers/81.pdf26 Jul 2013: Fluid Mech. 24, 313–358 (1992). 071904-16 Y. Man and E. Lauga Phys. ... Soft Matter 7, 8169–8181 (2011).24 L. Zhang, K. E. Peyer, and B. -
A smooth future?
www.damtp.cam.ac.uk/user/lauga/papers/51.pdf26 Jul 2013: be. L. L. a. V(z). Wetted. 0 s. 0 s. 24.5 s. ... Phys. Rev. Lett. 96, 186102 (2006).23. Squires, T. M. Phys. Fluids 20, 092105 (2008).24. -
Hydrodynamic friction of fakir-like superhydrophobic surfaces
www.damtp.cam.ac.uk/user/lauga/papers/42.pdf26 Jul 2013: J2k1/2(2πMa) cos 2kψ cos 2nψ (k 0). (2.24). Equation (2.24) is a symmetric infinite system of linear equations for the coefficients{cn; n 0}. ... The correspondingsolution of (2.24) is. c0 =4a. 3π. DL, cn = 0 (n > 0), (2.29). -
Flapping motion and force generation in a viscoelastic fluid ...
www.damtp.cam.ac.uk/user/lauga/papers/24.pdf26 Jul 2013: One such model is con-sidered in the discussion FENE-P, and we obtain the sameresults see also 24. ... S. Suarez and X. B. Dai, Biol. Reprod. 46, 686 1992.24 E. -
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. -
Soft Swimming: Exploiting Deformable Interfaces for Low Reynolds…
www.damtp.cam.ac.uk/user/lauga/papers/21.pdf26 Jul 2013: 9500 Gillman Drive, La Jolla California 92093-0411, USA(Received 15 January 2008; published 24 July 2008). ... J. Pedley and J. O. Kessler, Annu. Rev. Fluid Mech. 24,. -
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. -
Shaking-induced motility in suspensions of soft active particles…
www.damtp.cam.ac.uk/user/lauga/papers/35.pdf26 Jul 2013: By scaling timesby 9. 5122f 24 / 21 and numbering the particles along the. ... 24 and 25 to ex-plicitly obtain at leading order in 1 / di j. -
PHYSICAL REVIEW E 84, 031924 (2011) Fluid transport by ...
www.damtp.cam.ac.uk/user/lauga/papers/58.pdf26 Jul 2013: 2010).[19] S. Camalet and F. Jülicher, New J. Phys. 2, 24 (2000). ... Phys. 46, 13 (1997).[24] T. R. Powers, Rev. Mod. Phys. 82, 1607 (2010).[25] L. -
Propulsion in a viscoelastic fluidEric Laugaa� Department of…
www.damtp.cam.ac.uk/user/lauga/papers/18.pdf26 Jul 2013: Received 20 March 2007; accepted 16 May 2007; published online 24 August 2007. ... 083104-2 Eric Lauga Phys. Fluids 19, 083104 2007. Downloaded 24 Aug 2007 to 128.54.43.238. -
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] -
J. Fluid Mech. (2012), vol. 705, pp. 120–133. c� ...
www.damtp.cam.ac.uk/user/lauga/papers/69.pdf26 Jul 2013: Langmuir 24, 12158–12163.BATCHELOR, G. K. 1972 Sedimentation in a dilute dispersion of spheres. ... Annu. Rev. Fluid Mech. 24, 313–358. PHONGIKAROON, S., HOFFMASTER, R., JUDD, K. -
Propulsion by passive filaments and active flagella near boundaries…
www.damtp.cam.ac.uk/user/lauga/papers/43.pdf26 Jul 2013: F =1. 4. y02ISp. Sp4, 24. where ISp is a dimensionless integral defined by. ... 24, the measure-ments would show a decrease in the propulsive force nearboundaries. -
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 -
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. -
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.
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