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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). -
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. -
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. -
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.
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