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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 -
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. -
3C10b.dvi
www.damtp.cam.ac.uk/user/examples/3C10b.pdf26 Feb 2017: Cop. yrig. ht. 201. 7 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Quantum Fluids: Example Sheet 2. Problem 1. Mixtures of condensates. Consider a mixture of two different species ofbosons -
Journal of Integrable Systems (2016) 00, 1–13doi:…
www.damtp.cam.ac.uk/user/md327/CD16.pdf10 Jan 2017: where ξa are local coordinates on the fibres of M, and 24 is the Ricci scalar. -
The Electric Capacity of Suspensions of Red Corpuscles of a Dog
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Fricke1925.pdf11 Dec 2017: 93, 26.617. 93.710.26. 2.523. 20'. 22211480. 93.18.08—1. 93.6 93.710.68 10.72. 24. ... 24, 575-587 (1924},Eq. {13}. H. Fricke, The electric capacity of suspensions with special reference to blood,Jour. -
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) -
Comment on ‘‘Space-Time Crystals of Trapped Ions’’ In a ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Bruno2013b.pdf3 Dec 2017: L. Kuzemsky, Int. J. Mod. Phys. B 24, 835 (2010). [7] H. -
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]. -
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). -
Experimental evidence of a sustained standing Turing-type…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Castets_etal1990.pdf3 Dec 2017: 1990 The American Physical Society 2953. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990. ... Temperature: 7'C. 2954. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990. -
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 -
Impossibility of Spontaneously Rotating Time Crystals: A No-Go…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Bruno2013c.pdf9 Jul 2017: I; Xi. miR2. 1. hðiÞ;i. 1. ðiÞ;. 1. þ ðĥ2i; ĥi2;Þ > 0; (24). ... Phys. 5, 56 (2003).[24] I. Bloch, J. Dalibard, and W. Zwerger, Rev. -
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. -
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. -
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). -
PHYSICAL REVIEW FLUIDS 2, 093101 (2017) Two-fluid model for ...
www.damtp.cam.ac.uk/user/lauga/papers/140.pdf7 Nov 2017: 0.95 3.58–3.68 14.5 μm (1.9–4.3) 103U/U0 0.99 6.24–6.30 25 μm (1.3–2.6) 104U/U0 0.999 ... 0.049U/U0 0.95 3.58–4.04 15.2 μm 0.0020–0.022U/U0 0.99 6.24–6.91 26.3 μm (0.34–4.2)
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