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19 Dec 2012: 20 • • 21. «O κύριος λόγος που αποφάσισα να εκφρα-στώ δημοσίως είναι το χρέος που νιώθω προς τη νέα γενιά», είπε, οδη-γώντας μας σε ένα από τα

20 Nov 2012: Please update your bookmark! Last revised by G. Del Zanna on 20-Nov-2012.

2 Sep 2012: m. A trace amount of surfactant (Tween 20)stabilizes the film without harming the cells. ... Solid (red) linesare instantaneous streamlines and velocity vectors are shown ona log scale [20].

3 Oct 2012: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Teaching. DAMTP Summer School on Fluid Dynamics of Sustainability and the Environment. Supplementary Reading (Biological Physics). The following is a collection of primary

2 Sep 2012: BIOPHYSICAL JOURNAL VOLUME 20 1977202. ing the intake by local stirring would appear to be prohibitive. ... BIOPHYSICAL JOURNAL VOLUME 20 1977. I. 204. DV2c - v grad c = 0, (28).

13 Apr 2012: Example: for eating. a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. ... Elastic liquids. Studied for 20 years. Well understood now? library of behaviour? –

13 Nov 2012: 0.5. 1. 1.5. 2. 2.5. 3. 0 5 10 15 20. ... 1.5. 2. 2.5. 3. 3.5. 0 5 10 15 20. V0.

20 Jun 2012: June 20, 2012. 1. Complex fluids. What & where? tooth paste, soup, ketchup, synthetic fibres,. ... a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. t.

13 Apr 2012: 0.0001. 0.001. 0.01. 0 5 10 15 20. t. Results for the model fluids Oldroyd-B and FENEExp: Liang & Mackley 1994 JNNFM. ... Elastic liquids. Studied for 20 years. Well understood now? library of behaviour? –

24 Sep 2012: 20. Flow past a sphere Lagrangian unsteady. Numerical Oldroyd-B. DragStokes. Uτ/L. ... a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. t.

3 May 2012: Fluid Mech. 1994. 0. 20. 40. 60. 80. 100. 0 0.5 1 1.5 2. ... 1. 2. 3. 4. 5. 6. 7. 8. 10 20 30 40 50 60.

12 Jul 2012: Similar vortex arrays have beenemployed extensively for example in percolation theory[20]. ... 20] M. B. Isichenko, Rev. Mod. Phys. 64, 961(1992). [21] R.

19 Jan 2012: 20 JANUARY 2012. 0031-9007=12=108(3)=038103(5) 038103-1 2012 American Physical Society. ... 20 JANUARY 2012. 038103-4. 23] The case A 0 is solved in E.

19 Oct 2012: While simulations of the full system (1) are possible[17–19], here we develop evolution equations for the pri-mary orientation moments [20–22]. ... 0 10 20 300. 0.5. 1. 1.5. 0. m = 1.

21 Oct 2012: Fluid Mech. 1994. 0. 20. 40. 60. 80. 100. 0 0.5 1 1.5 2. ... 1. 2. 3. 4. 5. 6. 7. 8. 10 20 30 40 50 60.

9 Nov 2012: It’s the culmination of more than 20 years work. Most of the big breakthroughs were made in 1665 when Cambridge closed due to the plague and Newton returned to his

15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24]. ... Magnetic Suscepibility. -40. -20. 0. 20. 40. 0 1 2 3 4 5.

5 Dec 2012: 1 BTN = 2 (integration). 2 BAH = 1. Set r = 2π/20.

16 May 2012: A numerical plot of solutions of (3.20) for different γ1 is displayed inFig. ... Stud. Pure Math. 18-II (1990) 137. (1990).[20] D. Harland, T.A. Ivanova, O.

27 Dec 2012: 0. 5. 10. 15. num. ber. of c. olon. ies. Frequency15 20 25 30 35 400. ... Phys. J. E 34, 42 (2011).[20] N. Uchida and R. Golestanian, Phys.

23 Jan 2012: All algebraic curves in this class are projectively equivalent tothe rational cuspidal curves (5.20). ... The stabiliser of (5.20) is the one-dimensional group ofmatrices. aq2 p 0 0.

17 Apr 2012: s=1= 0. (2.20). There still remains the question of which modes µ to sum over. ... Phys. Fluids 20,063301. PICKARD, W. F. 1972 Further observations on cytoplasmic streaming in Chara braunii.

3 Oct 2012: 9), which occurs be-tween both charged (14) and uncharged (1) bilayers when d,< 20 A, has an important influence on contact and fusion oflipid vesicles. ... 1972) J. Colloid Interface Sci. 40,917-923.20. Alvarez, 0. & Latorre, R.

16 Jul 2012: we may pass to the limit in (3.19)-(3.20) andobtain that. ... J. Math.Imaging Vision, 20 (2004), pp. 89–97. [12] A. Chambolle and P.-L.

27 Nov 2012: 5.20). It is useful to introduce the adjoint operatorA via the Riesz representation theorem:first of all let. ... Theorem 5.3.3 Maximal monotone symmetric operators are self-adjoint. Theorem 5.3.4 (Stone theorem)If A is a self-adjoint operator the

2 Sep 2012: 2. y20,. with y0 20 mms.Visual observation showed that for small densities bac-. ... In gen-eral one may write y2rmsy. 20 aRb , where a is some.

3 Sep 2012: Scale bar in (a) is 2cm. Douglas [20] of minimal surfaces spanning a given contour. ... J. Mod. Phys. A 20 1252–59[13] BurnierY,WeberC,FlamminiAandStasiakA2007Local selection rules that candetermine specificpathways.

2 Sep 2012: 2Department of Physics, Haverford College, Haverford, Pennsylvania 19041, USA(Received 25 June 2009; revised manuscript received 20 October 2009; published 5 November 2009). ... A relatively dilute suspension of cells (5 106 cm3) ingrowth medium was

10 Oct 2012: 12], after the developmentof Young measures and weak convergence methods for partial differential equa-tions [13, 20]. ... 1 when t τ < t. (2.20). With this choice of θ, (2.19) reads.

2 Sep 2012: linearly, then more rapidly, and thenessentially linearly again, leading to shear thinning [20].If we switch on activity, with a positive value of W, therapid increase in Q implies an equally ... M. Goldbart, Phys. Rev. A 46, 4966. (1992).[20] P. D.

2 Sep 2012: 2] H. C. Berg and E. M. Purcell, Biophys. J. 20, 193 (1977).[3] J. ... Dombrowski et al. (to be published).[20] Somewhat similar patterns appear on agar substrates;.

12 Sep 2012: The dispersion medium may be a simple liquid or acomplex fluid itself (a polymer solution for instance) [20].The packing density is approaching the jamming situa-tion. ... J. E 15, 97 (2004).20. H. Van Damme, S. Mansoutre, P.

28 Feb 2012: 0.552. 0.554. 0.556. 0 5 10 15 20 25 0. 1. ... 35–52. << /ASCII85EncodePages false /AllowTransparency false /AutoPositionEPSFiles true /AutoRotatePages /None /Binding /Left /CalGrayProfile (Dot Gain 20%) /CalRGBProfile (sRGB IEC61966-2.1)

2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11. ... Two datasets are shown: 1 L = 20 cm, D = 0.5 mm, and a0 = 0.435 rad; 2L = 18 cm, D = 0.61 mm, and a0 = 0.814 rad.

2 Sep 2012: 12x). To test this model, we measured the f low fields aroundcolonies using methods described elsewhere (4), building onearlier studies (19, 20) and summarized in Methods. ... J. 20, 193–219. 13. Senft, W. H., Hunchberger, R. A. & Roberts, K.

2 Sep 2012: 20 JANUARY 2012. 0031-9007=12=108(3)=038103(5) 038103-1 2012 American Physical Society. ... 20 JANUARY 2012. 038103-4. 23] The case A 0 is solved in E.

16 Jul 2012: 20 ‘wraparounds’ for the function u(x) = ecos πx and N = ω1/2. ... 102. 103. 104. 105. 10-30. 10-25. 10-20. 10-15. 10-10. 10-5. ω.

2 Sep 2012: k̂?k̂, where k̂? is any unit vectorperpendicular to k̂. The dispersion relation for these modesis given by [20]. ... the aggregation of particlesby their swimming velocity in regions of rx cn< 0[20].

22 Mar 2012: 13, 18, 19, 20, 21, 25, 26].Assuming that f :RRd Rd satisfies the Lipschitz condition, the classicalwaveform Picard algorithm states. ... Sci. Stat. Comput., 8 (1987), pp. 459–482. 20. O. Nevanlinna, Remarks on Picard–Lindelöf iteration.

2 Sep 2012: Theirspeeds obey a messy cubic equation which, we can show[20], has real solutions for a finite range of parametervalues. ... These, as wellas other results on SPP nematics on substrates and ananalysis of isotropic SPP suspensions [3], will appear

2 Sep 2012: 20 30 40 50 60. rw[µm]. 10 1. 10 2. 10 3. ... 20, 0.03% vv) is added to the mixture to lowerthe surface tension of the cell suspension.

28 Feb 2012: Thus, for n = 0. 20. Figure 4.3: log10 |f̂[M]n f̂| for fc. ... Comput. Harmon. Anal. 20, 3–25. Iserles, A. (2011), ‘A fast and simple algorithm for the computation of Legendrecoefficients’, Numerische Mathematik 117, 529–553.

2 Sep 2012: The large differencein organism size between Volvox and Chlamydomonasrequired two distinct methods to measure the flows theycreate [20]. ... 95, 204501 (2005); D.Saintillan and M. J. Shelley, Phys. Fluids 20, 123304(2008); T.

2 Sep 2012: Velocimetry measurements were performed on a Bruker Spectrospin DMX 200,4.7 T magnet with a 20 mm long solenoid coil of diameter 3 mm; 1H images wereacquired at 199.7 ... 400 –200 200 4000 –40 –20 20 400. Position (μm). x (μm).

2 Sep 2012: Received 5 July 2003; revised manuscript received 20 January 2004; published 4 June 2004). ... Each flagellum consists of arotary motor; a universal joint about 50 nm long, known asthe hook, and a helical filament 20 nm in diameter and about10 mm long.

20 Oct 2012: 11. 10 20 30 40 50. 10-14. 10-11. 10-8. 10-5. 0.0120 40 60 80 100. ... 10-14. 10-11. 10-8. 10-5. 0.01. 20 40 60 80 100. 10-10.

2 Sep 2012: a5. 20. cossvtd. 1 L 24s4 2 6ad sinsvtd 1 O sL 4d ,ytorque. ... Schliwa, J. Cell Sci.109,509 (1996). [20] R. E. Goldstein and S.

27 Aug 2012: Putting y. (18). equation (16) gives. or. (20). (21). This represents a progressive wave of bending moment with a wavelength,velocity and direction of propagation similar to the wave of displacement;

11 Jul 2012: 0.87 2.22 0.11Qwater4 7.5 0.01 36.06 0.20 2.22 0.11Qethanol1 2.36 0.01 8.60 0.51 7.64 0.25.

2 Aug 2012: Wecan circumvent this problem if we consider instead the splitting. H̄(q, p, qt, pt) =. (1. 2p>p. )γ. (V (q) pt. )γ. (20). Separable Hamiltonian with kinetic energy quadratic in ... 20 Sergio Blanes, Arieh Iserles. 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.22.