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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.

24 Apr 2013: models for active systems have beenproposed [2, 17–24], but most of them have yet to be tested against experiments [14, 25]. ... where. M =(. 2 A 00 0. ) (0|k|2 2|k|4 i λ0kxv0)I (24).

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

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.”

26 Jul 2013: wall and crash into it. Furthermore, the authors proposed a. Submitted June 24, 2005, and accepted for publication September 28, 2005. ... xx Þ! ; (24). which is very similar to that given by the simple physical.

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.

4 Oct 2013: Xn(x) = Bn sinnπx. Lλn =. n2π2. L2. (24). Note that the first set eq. ... 24) the timeequation gives. Tn(t) = Cn exp(Dn2π2. L2t). The general solution for θ̂ (with odd initial condition θ̂(x, 0)) is thus.

12 Nov 2013: 22 4.000000302 3.015609e-07 0.5011010 1.0482393. 23 4.000000147 1.467238e-07 0.4865479 1.0479823. 24 4.000000064 6.370571e-08 0.4341880 1.0530215.

26 Jul 2013: 9500 Gilman Drive, La Jolla CA 92093-0411, USA. (Received 11 January 2013; revised 13 March 2013; accepted 24 April 2013).

26 Jul 2013: m=0. (q m)!(α1,0ρ). m m!(q m)! ), (3.24). 12 S. Michelin and E. ... general solution takes the same form, see (3.24). By matching c̃p, C̃p and C̃0 up to O(ε3/2), the values of b̃0, ãp and ap can then bedetermined, and