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26 Jul 2013: 4 6 1 1 13 24 1 1 21 40 1 15 6 1 3 14 28 3 1 22 42 1 16 12 3 1 15a 30 3 1 23 ... 43 2 37 12 1 1 15b 30 3 1 24 60 15 18 16 3 1 16 32 3 1 25 48 1 19 18 3 1 17 34 3

26 Jul 2013: Ishida et al.[21]. Tyrrell and Attard[22]. Tyrrell and Attard[23]. Steitz et al.[24]. ... These sizes are in agreement with the ex-perimental evidence of bubbles in Refs.[21–24], as summa-rized in Table I, although somewhat smaller.

3 Oct 2013: 093 —sea urchin (Lytechinus) 22.6 µm 4.6 µm 0.203 5.86sea urchin (Psammechinus) 24 µm 4.0 µm 0.166 —protist (Trypanosoma cruzi) 3.5 µm 0.5

26 Jul 2013: 4,5,24–30]. The individual locomotion of spermatozoa was first studiedby G. I. ... 24). The complete solution of the Stokes equations in cylindricalcoordinates to the first order in kb is therefore finally given by.

4 Oct 2013: u,Av) = (Bu,v) (24). (as you can easily check using the property that (Bu)† = u†B†). ... 36) of the µn values.). 1B Methods 24. 2.5 Parseval’s identity and least square approximations.

5 Oct 2013: R. Driscoll, “Wavelet-encodedMR imaging,” Magn. Reson. Med., vol. 24, pp. 275–287, 1992.

5 Oct 2013: xm} is a grid of mequispaced points in [1, 1]. In [24] it was shown that. ... Proc. SPIE, 7535, 2010. [24] D. Coppersmith and T. Rivlin. The growth of polynomials bounded at equally spaced points.

4 Oct 2013: G(x,t; ξ,τ) =H(c(t τ) |x ξ|). 2c. (24). (Note that this expression already requires tτ > 0 for G to be non-zero so we need notinclude

4 Nov 2013: 10 7.37 0.01 401 21.8 1.73 11111 6.63 0.01 401 20.7 1.69 10912 20.35 0.03 401 36.2 2.24 144.

26 Jul 2013: Following classical modelingapproaches [22–24], the deviatoric stress τ can be splitedinto two components, the viscous solvent stress (τ s ) and thepolymeric stress (τ p); τ s is thus given by. ... 1: Fluid Mechanics 2nd ed. (WileyInterscience, New