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October 2016 EPL, 116 (2016) 24002 www.epljournal.orgdoi:…
www.damtp.cam.ac.uk/user/lauga/papers/127.pdf8 Nov 2017: I 1. 2ezez. ). (I ezez) = I, (24). and we further note that ξ/4πµ 1/ln(1/ϵa) [9]. ... Rev. Lett., 96 (2006). 058102.[24] Guirao B. and Joanny J. F., Biophys. -
Big Issues for the Cambridge Area What kind of ...
www.damtp.cam.ac.uk/user/pvl/2050/reportfinal.pdf19 Dec 2017: Quality of life 16-24 year-olds complain of not enough to do, and that the events and. -
Traces of surfactants can severely limit the drag reduction of…
www.damtp.cam.ac.uk/user/gold/pdfs/Traces.pdf12 Jul 2017: 25 and 38 have gas fractions 26–55%; the gratings in ref.24 have g '1 mm). ... Phys Fluids 24:112003. 24. Bolognesi G, Cottin-Bizonne C, Pirat C (2014) Evidence of slippage breakdown for asuperhydrophobic microchannel. -
PHYSICAL REVIEW FLUIDS 2, 034201 (2017) Autophoretic flow on ...
www.damtp.cam.ac.uk/user/lauga/papers/134.pdf13 Mar 2017: 2′. n=0 fn d. 2. 2(U α β). (24). Finally, to determine U , we impose that the force on the torus must vanish. ... 100 100.5 101. 0.24. 0.245. 0.25. s0. |U|. 0.8 1 1.2Concentration. -
Manton’s five vortex equations from self-duality
www.damtp.cam.ac.uk/user/md327/CD_vortex_published.pdf23 Aug 2017: T =AreaN8π2. Σ. [2. ȧwȧw Cφ̇φ̇]ωΣ, (3.24). F Contatto and M Dunajski J. ... WN} is, from (3.24),. AreaN8π. Ni,j=1. ((Wk)δij 2Wi bj) dWidW j,. -
PHYSICAL REVIEW E 95, 062416 (2017) Empirical resistive-force theory…
www.damtp.cam.ac.uk/user/lauga/papers/138.pdf7 Nov 2017: small-amplitude perturbations of Taylor’s swimming sheet[24] and squirming motion on a spherical surface [26]. ... 15) in any shear-thinning fluid model. We choosethe Carreau model, which is a good fit to many shear-thinningfluids [24,52] and in -
PHYSICAL REVIEW E 94, 062606 (2016) Can phoretic particles ...
www.damtp.cam.ac.uk/user/lauga/papers/129.pdf8 Nov 2017: At large times, clearlythe time-independent terms in (24) can be neglected comparedto the logarithmic term. ... J. E 29, 27 (2009).[24] J. Brady, J. Fluid Mech. 667, 216 (2011).[25] B. -
Fokas Method (unified transform) January 25, 2017 1 Brief ...
www.damtp.cam.ac.uk/user/examples/3N15.pdf26 Jan 2017: where. û1(λ) eiλN1l=0. [iλal1P̂l(λ) b. l1P̂l(λ). ],. 24. û2(λ) eλN1l=0. [λal2P̂l(iλ) bl2P̂l(iλ). ],. ... Appl. Math. 24 (2013), no. 6, 857–886, DOI10.1017/S0956792513000223. MR3181485. [24] B. -
J. Fluid Mech. (2016), vol. 796, pp. 233–256. c© ...
www.damtp.cam.ac.uk/user/lauga/papers/118.pdf3 May 2017: 8 24.2Re(c2) Re(c1) 93 96 40 12.3 7.5 3.2. ... In (a) Re = 21.7and (b) Re = 24.0, Re(c1) < Re < Re(c2), and a constant steady-state lift force is observed.In (c) Re=25.3 and (d) -
Chapter 8Theory of Locomotion Through Complex Fluids Gwynn J. ...
www.damtp.cam.ac.uk/user/lauga/papers/98.pdf23 Nov 2017: 8.17) dictates that. V#̇ : ûdV = 0, (8.24). and so the velocity of the swimmer, as given by Eq. ... experimental measurement of the swimming kinematics ofdeforming bodies [24] based on theory proposed by Khair and Squires [23]. -
Geometric tuning of self-propulsion for Janus catalytic particles
www.damtp.cam.ac.uk/user/lauga/papers/133.pdf8 Nov 2017: and on the interaction between the surface of the particle and its physico-chemical environment (M)24. ... Designing phoretic micro- and nano-swimmers. New J. Phys. 9, 126 (2007).24. -
Electrodynamics Michaelmas Term 2016 Lecture notes Anthony…
www.damtp.cam.ac.uk/user/examples/D21Lb.pdf9 Oct 2017: 3.24)The solution of Eq. (3.23) with initial condition uµ = uµ(0) at τ = 0 is. ... 4.24) by a term. 1µ0c. αAµFνα = 1. µ0cα (AµF. να) , (4.45). -
Three-body interactions, scaling variables, and singular diameters in …
www.damtp.cam.ac.uk/user/gold/pdfs/3body.pdf19 Dec 2017: T(x) = —', p(x)[1 —xp(x)][1 ——,'p(x)]. 1/2. (23). (24). (25). (26). -
Magnus expansions and pseudospectra of Master Equations
www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_01.pdf11 Jan 2017: X = tp 12t2[p,k] 1. 6t3[k, [p,k]] t4. (1. 24[p.[p, [p.k]]] 1. ... 24[k, [k, [p,k]]]. )(20)265. t5(. 7. 360[k, [p, [p, [p,k]]]] 1. -
J. Fluid Mech. (2017), vol. 812, R3, doi:10.1017/jfm.2016.807 Helical …
www.damtp.cam.ac.uk/user/lauga/papers/130.pdf8 Nov 2017: Phys. Fluids 24, 081703.LAUGA, E. 2007 Propulsion in a viscoelastic fluid. ... 2012 Self-propulsion in viscoelastic fluids: pushers vs. pullers.Phys. Fluids 24, 051902. -
Noname manuscript No.(will be inserted by the editor) Uniform ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2014_04.pdf14 Jun 2017: ckBλ ,1(ck,t)dt, (23) ck1. ck. t1ck. [Bλ ,1(ck,t2),Bλ ,1(ck,t1). ]dt2dt1, (24) ck1. ... of (24)to local order 8 is equivalent to quadrature of (35) to local order 3,. – -
rspa.royalsocietypublishing.org ResearchCite this article: Cooray H,…
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Cooray-2016.pdf20 Jan 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... angles. SIAM J. Appl. Math. 49, 1009–1028. (doi:10.1137/0149061)24. Vogel TI. 2013 Liquid bridges between balls: the small volume instability. -
31.tif
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Gates1930.pdf11 Dec 2017: r 24 25 26 21.28.29.30.31. 22.23 24 25 26 21. 28 29. ... z2.1 o. r-. o or5. 12. %. 6. 022. 23 24 25 26 27 28 29. -
on November 22, 2017http://rsif.royalsocietypublishing.org/Downloaded …
www.damtp.cam.ac.uk/user/lauga/papers/142.pdf22 Nov 2017: Ð L0 k. 2(s, t)ds, with a vanishing intrinsic curvature[24], thus neglecting shearing stresses. -
PHYSICAL REVIEW FLUIDS 2, 084101 (2017) Analytical solutions to ...
www.damtp.cam.ac.uk/user/lauga/papers/139.pdf7 Nov 2017: This understanding has then prompted the scientificcommunity to create artificial microswimmers [22–24]. ... 24)The above force exhibits a structure 1/[ln(/b) ξ ], where ξ is some constant, very similar to theforces exerted by a thin prolate ellipsoid
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