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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.

3 Jan 2013: S-shaped actuation [24] and asoft three-link manipulator with visual feedback [25]. ... frame sequence number17 21 24 1 5 9 13. frame sequence number17 21 24.

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: 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.

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

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

19 Oct 2013: For example, when the TearDrop IP attack was first posted to the web, less than 24 hours passed before the Linux community had a working fix available for download.

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: 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.

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: Thesecond mode (n2) defines the local stress applied by theswimmer on the surrounding fluid.8,24. ... cðr; lÞX1m0. CmðrÞLmðlÞ: (26). Substituting Eq. (26) into Eqs. (24) leads after projection on.

26 Jul 2013: We also plot in Fig. 3 the results ofour model for both surface coverage considered in the twoprevious studies: = 0.43 dashed line and = 0.68 solidline.24.

26 Jul 2013: Flexible propeller10L 24 mm. Umax z 94 f 10 HzU z 22 mm s1a. ... The dimensionlessboundary conditions are. N(s 0) 0, (24). M(s 0) 0, (25).

26 Jul 2013: h2. 2 ̄. 3 ̄ ̄̄. 24. III. RELEVANCE TO GASTROPOD CRAWLING:IMPACT OF RHEOLOGY ON LOCOMOTION COST. ... Zool. 24, 231984. 27M. W. Denny, “Invertebrate mucous secretions: Functional alternatives tovertebrate paradigms,” Symp.

26 Jul 2013: F (r ) = C1 Iλ(kr ) C2 Kλ(kr ), (24). ... Applying the condition that p̂ is finite at r = 0 to equation (24)eliminates Kλ as a solution for F.

26 Jul 2013: 24 represents aweak constraint on the validity of neglecting forces from theintermediate region. ... Furthermore, more systematicobservational studies are needed to identify which watersnail species exhibit which modes of “inverted crawling.”

19 Oct 2013: 24. The oldest strain of such non-conformism is Calvinist, Puritan.

29 May 2013: Although very dif-ferent in size and composition, these systems are oftenjointly termed ‘‘active’’ fluids, for which there is now arange of continuum theories [12,14–24]. ... 2(d)] we observe the linear scaling z Exy=2,with 24 m being roughly