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19 Dec 2017: Quality of life 16-24 year-olds complain of not enough to do, and that the events and.

12 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.

13 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.

8 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.

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,.

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

26 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.

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)

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.

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].