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24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 424 E. J.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 804 E. J.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meck. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 292 E. J.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meoh. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 470 H. A.

8 Jul 2009: 1–24 of the Collected Papers, Vol. 3, M. Y. Hussaini, Ed., Oxford.

14 Jul 2009: Quite clearly the time-step 6 t = 0.03, with the large random displacement (2D6t)'l2 = 0.24, smears out the details which are to be resolved.

30 Nov 2009: 24 H. Brunner, A. Iserles & S.P. Nørsett. Figure 3.3: The number of significant digits in approximating one of the two nonzero eigen-values forKω(x, y) = cos ω(x

14 Jul 2009: http://journals.cambridge.org Downloaded: 14 Jul 2009 IP address: 131.111.16.227. J. Fluid Mech. (1996), t d 308, p p. 255-288 Copyright @ 1996 Cambridge University Press. 255. Computer simulations of polymer chain relaxation via Brownian motion. By

10 Jul 2009: B. PerrinLaboratoire de Physique de la Matiere Condensee, UMR 8551, CNRS, Ecole Normale Superieure,Département de Physique, 24 rue Lhomond, 75231 Paris Cedex 05, France.

21 Apr 2009: Multivariate modified Fourier series and application to boundary. value problems. Ben AdcockDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, Cambridge CB3 0WA. United Kingdom. March 25, 2009. Abstract. In this paper we

12 Aug 2009: 12α2 (1 α)2 ‖y. j xk‖4, αR, (4.24). the last line being due to the positive semi-definiteness of =ZZT.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 686 L. G.

23 Jul 2009: http://journals.cambridge.org Downloaded: 23 Jul 2009 IP address: 131.111.16.227. J. Fluid Mech. (1977), vol. 83, part 4, p p. 695-720. Printed in Great Britain 695. An averaged-equation approach to particle interactions in a fluid suspension. By E.

10 Nov 2009: Received 8 June 2009; accepted 3 August 2009; published online 24 September 2009.

10 Jul 2009: The pairs were then processed to find tvelocity-vector map of the flow field by using an adaptsource code and compiled application for PIV developedCardoso.24.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Pluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 746 L. G.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... 3A(sin4 8, sin 24,) - 2(A - B)(sin28, sin 24,)}, of, = of. =

20 Sep 2009: Employment has fallen 24,000 in the last quarter. Unemployment now 6.5 per cent (4.6 per cent a year ago).

20 Sep 2009: you will help save paper. Responses needed by Tue 24 November 2009.

28 Sep 2009: Equations, 30 (4), (2007), 523–546.24 pages. ... 24. D. Stuart, “Perturbation theory for kinks”, Communications in Mathematical Physics,149 (1992), 433-462.

16 Jan 2009: n E|. =1. ǫ0σ (23). nE|. = 0. (24). b). Let S carry current density s per unit length (charge crossing unit length in S in unittime).

29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to.

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

15 Oct 2009: 2ψ22) 2me2N Φ21. (e2N 1)2. 2me2Nψ22 4. rΦ1ψ2. = O(1),. (1.24). ... To see this, observe that by (1.24) and the preceding remarks, the equationF(l,Q,N, Φ1,ψ2; 0) = 0 amounts to.

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

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.

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.

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.

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,.

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).

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.

10 Jul 2009: For the same trial as in Fig. 5, this constantB is found to be20.90 and 24.29 for the large andsmall angle sides, respectively.

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.

31 Jul 2009: SZAN-IAWSKI, A. 1972 Arch. Mech. 24, 555. TANNER, R. I. 1971 J.

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.

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.

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.

13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C.

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

8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.

13 May 2009: Van,cn(α, β, nz) =. 0(t α)a(t β)cenφ(t) dt, (4.23). withφ(t) = zt log(t α) log(t β) (4.24). ... Iserles (DAMTP, University of Cambridge). 24. References. [1] Milton Abramowitz and Irene A.

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.

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

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.

1 Dec 2009: 3.24). The corresponding result is the following. Theorem 2 Let f(y) be constant, then we have θ0 = 0, θ1 = ̺ and. ... θs = (s 1)̺, s 2.Proof We shall use formula (3.24) and proceed along the lines of theproof of Theorem.

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

23 Jul 2009: 7 2 13.3 19.7 34.0 % / a , 1.33 1.64 2.13 2-55 3.63 4.24 5. ... Even for r = 30 a 24 Yo variation from axisymmetry produces a drift in 6 from &7r to approximately.

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].

8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.

8 Jul 2009: 2 a1.02r30. In both geometries, the final slope at the front is much lower than the slope thatwould be given by an internal angle of friction δ = tan1(µ) = 24.