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23 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,.

8 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.

7 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

27 Oct 2017: Old people in Cambridgeshire. 2012 2030? Over 65 96,000 17%. 135,000 24%.

8 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.

10 Jan 2017: where ξa are local coordinates on the fibres of M, and 24 is the Ricci scalar.

3 Dec 2017: L. Kuzemsky, Int. J. Mod. Phys. B 24, 835 (2010). [7] H.

11 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.

3 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)

23 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].

3 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.

19 Dec 2017: T(x) = —', p(x)[1 —xp(x)][1 ——,'p(x)]. 1/2. (23). (24). (25). (26).

9 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.

22 Nov 2017: Ð L0 k. 2(s, t)ds, with a vanishing intrinsic curvature[24], thus neglecting shearing stresses.

7 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

11 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.

20 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.

14 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,. –

11 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.

9 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).