Search

31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

27 Jul 2009: 4.25)We now consider the reduction of the system (4.23),(4.24). Theorem 1.1 arises as acorollary of Proposition 4.2. ... to a coupled system whichincludes the Z3 two dimensional Toda chain [24] as a special case.

17 Sep 2009: It has been developed over the last30 years by the Oxford school of Penrose and Atiyah with the crucial early input from Ward[24, 25] and Hitchin [10, 11] and further ... Sächs. Akad. Wiss. Leipzig, Maths. Nat. Kl 69 262–77[24] Ward R S 1977 On

15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details.

30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future.

13 Jul 2009: Lipscombe, R. Kennings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85 [l]). ... References. 1 G.G. Lipscomb, R. Keunings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85-96.

26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-.

24 Feb 2009: µe = 0.47 for centre of massIC 2009, runout – p.24/59.

10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7.

23 Jul 2009: The differential equation can be integrated directly taking Po = 24 to produce an implicit expression for the shape. ... z = 0s-1 F 24( 1 - F2). which when substituted in the volume constraint yields.

8 Jun 2009: Calculation) method [24–26]. Although the THINC/WLIC method is a type of VOF method. ... for Fluid Dynamics, Morton KW, Baines MJ (eds) Vol. 24, Academic Press: New York, 1982; 273-.

10 Jul 2009: 1 O f 11/3! (24). Figure 3 shows the settling velocity for a simple cubic arrayspherical particles as a function off 1/3. ... It can be seen that thenumerical results, obtained by considering the finite size ofparticles, yield close agreement with the

3 Sep 2009: V|ψ|2 dx = ψ2u v, (24). where v =. V dx, and by ψ the wavefunction of the bulk: ψ ψ as r. ... For thequartic term in the expression for the energy, we write using equation (24).

10 Jul 2009: π2/24, 24/π) (0.4112, 7.639), although the numerical results suggestthat the analysis of 4 requires β 1 101 rather than β 1. ... 24/(βT ) (lower), wherein the factor 2 has been included to translate the lines.

14 Jul 2009: 0.24 1. 0.18. (T 0.12. 0.06. 0 a. FIGURE 2. The growth rate 0 = aci as a function of wavenumber CI for the varicose mode of a ... The dashed curves are contours of pressure. 0.24. 0.18. 0 0.12.

8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex, 05, France. ... Rev.Fluid Mech. 24, 21 s1992d. 12F. Viana, R. Pardo, R. Yanez, and J.

10 Jul 2009: For A60,with an initial capillary pressure of 0.76 times the total elastic modulus, a pre-stretch of 3 anda finite extension of L1 = 24 (cf. ... The continuous curves are (a) for A40,L1 = 77 and P = 5; (b) for A60, L1 = 24 and P = 3; (c) for A80 L1 = 4.5

16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

8 Jul 2009: σtotn = 1Ca. κn, on ΓM(t). (24). Since there is no fixed boundary in this problem, the purely.Lagrangian approach is well adapted to it. ... Non-Newtonian Fluid Mech. 110 (2–3)(2003) 77–102. [24] R.F. Liang, M.R. Mackley, Rheological

13 Jun 2009: The the extension to bivariate functions was developed, without analysis,in [24, 25, 27]. ... The bivariate version of this method wasoriginally developed, without analysis, in [24, 25, 27].