Search

26 Jul 2013: 072102-2 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012). ... 072102-5 G. J. Elfring and E. Lauga Phys. Fluids 24, 072102 (2012).

5 Oct 2013: J. Amer. Math. Soc., 24(1):81–124, 2011. 1.

26 Jul 2013: PHYSICS OF FLUIDS 24, 051902 (2012). Self-propulsion in viscoelastic fluids: Pushers vs. ... Fluid. Mech. 24, 313–358 (1992).3 N. A. Hill and T. J.

18 Jan 2013: iv) Integrable Nolinear Elliptic PDEs. J. Lenells and A.S. Fokas, Boundary Value Problems for the Stationary Axisymmetric Einstein Equations: A Rotating Disk, Nonlinearity 24, 177-206 (2011). ... iii) Gravitometry. V. Michel and A.S. Fokas, A Unified

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

26 Jul 2013: σ aux = 0, (23). uaux = 0. (24)Taking the inner product of Eq. ... d V. (30). 103102-9 Pak et al. Phys. Fluids 24, 103102 (2012).

5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps

26 Jul 2013: 24),simplifies to. F̂ 〈U2〉=. V0. 〈Σ[u1]〉 :ûdV. (26). 64001-p4. Life at high Deborah number. ... 24] Leal L. G., Annu. Rev. Fluid Mech., 12 (1980) 435.[25] Blake J.

20 May 2013: 2] Kapustin and Strassler, 9902033. 5. BZ la[ce spacing. 24 fermions! •

27 Feb 2013: Ann travels at a speed given. by β u/c = 24/25 in the x-direction for seven years and then comes back at the.

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.

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

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

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

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

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.

27 Aug 2013: pointed) end to its plus (barbed) end.These cables are bound to the cortically fixed chloroplasts atthe cell periphery (24) in a “barber pole” twist, generating flowspeeds of 50–100 ... Characean algae. Proc Natl Acad Sci USA 73(1):165–167.24.

19 Oct 2013: variable between about 24 and 36 months — owe their existence and timing to the ir-. ... cycle taking, of course, about 24 to 36 months. The time-altitude contour plot of the.

26 Jul 2013: 2, 0.5) (1.1, 0.4)f (2.2, 0.53) (0.91, 0.29)g (2.3, 0.45) (0.69,1.52) (1.24, 0.52) (1.14,

26 Jul 2013: 0 aRFU 0 , 24. Text = 0 0 00 0 aRFU0 aRFU 0. ... Optimal III 0.24 3.34 12.6 2.6 7.9 0.336. Optimal IV 0.49 3.20 16.9 2.6 5.4 0.465.

24 Jun 2013: 2Department of Physics, University of Arizona, Tucson, Arizona 85721, USA(Received 10 April 2013; published 24 June 2013). ... Stocker,Phys. Fluids 24, 091107 (2012). [28] W. R. DiLuzio, L. Turner, M.

26 Jul 2013: J. Fluid Mech. (2003), vol. 489, pp. 55–77. c 2003 Cambridge University PressDOI: 10.1017/S0022112003004695 Printed in the United Kingdom. 55. Effective slip in pressure-driven Stokes flow. By ERIC LAUGA AND HOWARD A. STONEDivision of Engineering

16 Oct 2013: m=1. α(m)(t)δmn. = α(n)(t) , (1.24). reproducing (1.23) apart from renaming the indices. ... 24. Chapter 2. 2. Groups. This chapter contains the second set of syllabus items, together with a fewitems anticipating the third set:.

26 Jul 2013: Other simple propulsivesystems proposed for locomotion at zero Reynolds numberinclude a deformable two-dimensional loop;18 systems oftwo,19–22 three,21,23,24 or N spheres;25 an oscillating body ... R2. z c. R1, 24. where c = a2 b2, r = x2 y2, r̂ =

12 Aug 2013: Cont. Dynamical Sys. 28, 1345–1367. 24. Figure 3.4: The errors for h(t) for ω = 200π (top row) and ω = 2000π(bottom row): from the left 0, 1 and

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 Nov 2013: Leakage. † Present address: Department of Mechanical Engineering, MIT, Cambridge MA 02139, USA.‡ Present address: OCCAM, Mathematical Institute, 24-29 St Giles’, Oxford OX1 3LB, UK.

19 Oct 2013: Fluid. Dyn. Res., 24, 375–404.Janssen, P. A. E. M. 1982 Quasilinear approximation for the spectrum of wind-generated.

9 Jan 2013: N 2)(7N 11)ρ (N 1)(7N2 27N 24)ρ2. (N 3)(N 2)(2N 1)ρ3],.

8 Jun 2013: simulations. g, North Atlantic sediment core OCE326-GGC5 231Pa/230Th (ref.24). Temperatures are given as deviations from the early Holocene (11.5–6.5 kyr ago) mean. ... Paleoceanography 18, 1087 (2003). 24. McManus, J. F., Francois, R., Gherardi, J.-M.,

4 Nov 2013: Fluids 24, 117102 (2012) Effect of fluctuations on the onset of density-driven convection in porous media Phys. ... Fluids 24, 114102 (2012) Absence of subcritical instabilities and global nonlinear stability for porous ternary diffusive-convective

4 Nov 2013: φ̃0(0; λ̄) =. h(0, y)2 dy. (3.24). The solid curve in figure 5 shows the result of substituting the value of φ̃0(0; λ̄)found in this way

4 Nov 2013: FC = 24/3λD. (gβ̃. Dν. )1/3(C0 Ci )4/3, (4.3). where λ is a constant. ... 1 9.3 0.1 9 1 10.47 3.73 0.25 unstable230106D 9 1 3.19 0.02 27 0.3 10.47 3.73 0.24 unstable230106E

26 Jul 2013: CA 92093-0411, USA2LadHyX, École Polytechnique-CNRS, 91128 Palaiseau Cedex, France. (Received 28 April 2003 and in revised form 24 March 2004). ... By selecting ξinf = 15.7 andξsup = 24 and defining N = 140 gridpoints via this approach, adequate

26 Jul 2013: Received 24 May 2002; accepted 17 December 2002; published online 30 June 2003.

4 Nov 2013: j r)2 α2][(j r)2 (j r) α2 ϵ1]aj. = ϵ1[α2 1 (j r 1)2]aj1, (24). ... book. Of particular relevance to this analysis arethe studies of the hydrodynamic stability of the asymptotic suctionprofile by Hughes and Reid [23], Hocking [24] and Lakin andReid

26 Jul 2013: to the cre-ation of flagella bundles propelling the cells forward as theyswim, as well as the disruption of such bundles when thecells change their swimming direction.22–24. ... U =h̄. 2f x. s. 24. Noting that d / dt = U we therefore get an equation

26 Jul 2013: 24). If we note 〈.〉 the t -averaging operator between t and t 2π, we therefore obtain〈e(j )i. ... 27). From the definition of F and Eqs. (24)–(27), we can write.

5 Oct 2013: The second inclusion follows by Theorem VIII.24 ([RS72], p. 290)if we can show that PnAPn A in the strong resolvent sense. ... 11. Proof. Now, (i) follows from the fact that A1,n A strongly (see Theorem VIII.24 in [RS72],p.

5 Jun 2013: Charney [24], Aleksandr Mikhailovich Obukhov [25],. and Ernst Kleinschmidt [26]. 1.4 Cyclone and jet structure. ... dent pioneering work of Charney [24] and Obukhov [25] and are described.

5 Oct 2013: 3 Consistent reconstructions and oblique projections. We now consider the consistent sampling technique of [24, 25, 29, 56, 58]. ... An analysis of consistent reconstructions, which we shall recap and extend in 3.3, was given in[24, 25, 29].

19 Oct 2013: Solar tachocline dynamics: eddy viscosity,anti-friction, or something in between? MICHAEL E. McINTYRE. Centre for Atmospheric Science† at theDepartment of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce

5 Oct 2013: The well known NS-Sampling Theorem [24, 26, 29, 30, 34] states that if.

26 Jul 2013: have been investigated iRef. 24. P license or copyright, see http://pof.aip.org/pof/copyright.jsp.

7 Jan 2013: Photosynthetically Active Radiation (Fluora; OSRAM) and 10 h in dark at 24 C.Cells were harvested during the exponential growth phase. ... animal and plant functions. Science 318(5848):245–250.24. Fujiu K, Nakayama Y, Iida H, Sokabe M, Yoshimura K (2011

19 Jul 2013: Dynamical Sys. 28, 1345–1367. 24. Deaño, A. & Huybrechs, D. (2009), ‘Complex Gaussian quadrature of oscillatory in-tegrals’, Numer.

4 Nov 2013: Carbon budgets have been introduced to capemissions [24] (Figure 1). The power sector is the single largest emitter. ... and are designed to capemissions [24] (green line).