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3 Oct 2013: As a last example, we point out thatparticles diffusiophoretically transported by a homogene-ous solute gradient [24] should also display a very similarpropagative dynamics, as they also induce a weak far ... 23] A. M. Menzel, Phys. Rev. E 85, 021912

26 Jul 2013: 2. order OKn. Downloaded 24 Oct 2005 to 18.51.1.222. Redistribution subject to A. ... Kn O a3. h3. 38b. Downloaded 24 Oct 2005 to 18.51.1.222.

26 Jul 2013: or motion and we will thus not consider chemical swimmers21–24. or solid bodies powered by external fields.25. ... 24 G. Ruckner and R. Kapral, Phys. Rev. Lett., 2007, 98, 150603.25 S.

26 Jul 2013: c ðv2s=DRÞk2, as could havebeen anticipated from the single-swimmer problem [24].However, hydrodynamic interactions result in a renormal-ization of this single-swimmer effect. ... 24] J. R. Howse, R. A. L. Jones, A. J. Ryan, T.

26 Jul 2013: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

17 Dec 2013: δε = τλ‖. 〈Fy〉W 2tot. τ. 0δα H ( ḟ , f̈ , α, α̇, α̈) dt, (24). ... Rev. Lett. 93 186001. [24] Tabata O, Hirasawa H, Aoki S, Yoshida R and Kokufuta E2002 Ciliary motion actuator using self-oscillating gelSensors Actuators A 95 234–8.

26 Jul 2013: 24) is now triv-ial and the swimmer orientation remains constant. Sincethe flow is irrotational, no hydrodynamic torque (fromvorticity) is present to modify the orientations of the par-ticles. ... 23)and (24) and obtain. M =2μσπa3. M ′1 M′2 0. M

14 Aug 2013: Received: 24 April 2012 / Accepted: 20 November 2012Published online: 21 May 2013 – Springer-Verlag Berlin Heidelberg 2013. ... J. Math. Phys 18, 1449 (1977)24. Penrose, R.: Nonlinear gravitons and curved twistor theory.

26 Jul 2013: Typicalvalues for b range from $%1 for bacteria like E. coli,6 $0for Volvox and artificially created squirmers17,24,27 to $þ1for Chlamydomonas.19.

26 Jul 2013: Received 24 June 2003; accepted 11 February 2004; published online 1 July 2004! ... 24! Here we effectively demonstrate that these ideasalso apply as well to slowly varying flows.