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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

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].

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

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

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

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).

26 Jul 2013: Contents. Front Pages. Aboutthe Authors. Subject Index. UserInstructions. LicenseAgreement. Chapter 19 in Handbook of Experimental Fluid Dynamics,C. Tropea, A. Yarin, J. F. Foss (Eds.). Springer, New-York (2007), ISBN: 978-3-540-25141-5.

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 Oct 2013: π. L. L2 D2. As (y′) dy′. (4.24). This expression can be cross-checked by evaluating the y-components of the sourceand sink recoil forces in (3.6) to ... 5.24). The direction of RV is not, of course, exactly parallel to ŷ, but rather makes anO( 2)

21 Mar 2013: will show that. Proposition 1.1. The metrics Nil (3.24), Sol (3.27) and the generalised Berger. ... 23. 24 CHAPTER 2. PATH GEOMETRY. passing through a point is fully described by the direction of the tangent vector.

19 Oct 2013: The total number of two-note neighbours, with two notes invariant and the other two raised or loweredby a semitone, in all possible combinations, works out to be 24, not counting ... A single diminished seventh has 4, 4, 8, 4, and 4 different neighbours

19 Oct 2013: 9in x 6in lecturenotes˙190410. 16 P. H. Haynes. estimated by 1/3L2/3(122/3 24/3 κ1/2L2/31/6).

19 Oct 2013: u′1 u′1) = vS2 (β Uyy) (f Uy)uS2. (3.24)It can be checked that retaining the smaller advection term from (3.9) would only adda much smaller term ... than either of the two terms on the right-hand side of (3.24).

5 Oct 2013: The problem is not new, and therehave been many different approaches developed for its solution (see, for example, [2, 11, 12, 17, 18, 22,23, 24, 25, 52] and references therein).

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 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].

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

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

19 Oct 2013: 23 Nov 2004 1:27 AR AR235-FL37-11.tex AR235-FL37-11.sgm LaTeX2e(2002/01/18) P1: IBD10.1146/annurev.fluid.37.061903.175710. Annu. Rev. Fluid Mech. 2005. 37:263–93doi: 10.1146/annurev.fluid.37.061903.175710. Copyright c 2005 by Annual Reviews. All

27 Jun 2013: 2. 24. We now let s in (3.22),. lims. χs+ = lims. ... φm(z) =. mj=0. (1)mj[mj. ]q. q12 (mj)zj, m Z+. (3.24). Setting α = q1/2 presents absolutely no problems in our analysis, since q = |α|2, isconsistent

5 Oct 2013: Thiswas later considered by Eldar et al, who extended this framework to frames in arbitrary Hilbert spaces[18, 19, 20, 24]. ... M2 =. C(γ)M11. 2. (24). Proof. Without loss of generality, in this proof, M1 and M2 will be even.

20 Dec 2013: T(η,ω,X) = TabcηaωbXc. (2.24). This formula generalizes in the obvious way to a (r,s) tensor. ... Thisis easiest to demonstrate with an example. Part 3 General Relativity 4/11/13 24 H.S.

5 Oct 2013: Indeed, one typically requiresan intolerably large number of samples m to recover f to any reasonably accuracy [13, 24]. ... 24]. Note in the case above that f has only m nonzerocoefficients in the basis {wj}jN.

4 Nov 2013: 2011], but that it can be approxi-306 mated as constant provided that the thickness of the CO2307 layer is small relative to the thickness of the water layer.308 [24]

4 Nov 2013: J. Fluid Mech. (2010), vol. 647, pp. 287–308. c Cambridge University Press 2010doi:10.1017/S0022112009993910. 287. On the mechanisms of icicle evolution. JEROME A. NEUFELD†, RAYMOND E. GOLDSTEINAND M. GRAE WORSTER. Institute of Theoretical

19 Oct 2013: BALANCE, POTENTIAL-VORTICITY INVERSION, LIGHTHILL. RADIATION, AND THE SLOW QUASIMANIFOLD. M. E. McINTYRE. Centre for Atmospheric Science at theDepartment of Applied Mathematics and Theoretical Physics,Silver Street, Cambridge CB3 9EW,

5 Oct 2013: The problem is not new, and therehave been many different approaches developed for its solution (see, for example, [2, 11, 12, 17, 18, 22,23, 24, 25, 52] and references therein).

5 Oct 2013: Stable reconstructions in Hilbert spaces and the resolutionof the Gibbs phenomenon. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of

19 Oct 2013: 12 2 2 41 F f r 1 O(F lnF). 4(24). ... In particular, atO(1), this means that the coefficients of the lnr term in(18a) and (24) must agree, and hence.

5 Oct 2013: Thiswas later considered by Eldar et al, who extended this framework to frames in arbitrary Hilbert spaces[18, 19, 20, 24]. ... M2 =. C(γ)M11. 2. (24). Proof. Without loss of generality, in this proof, M1 and M2 will be even.

5 Oct 2013: Indeed, one typically requiresan intolerably large number of samples m to recover f to any reasonably accuracy [13, 24]. ... 24]. Note in the case above that f has only m nonzerocoefficients in the basis {wj}jN.

19 Oct 2013: 24. The expression (• • ••) for p(r, t) tell us something interesting about the way the pressure p(r) varieswithin the liquid; (••••) simplifies to.

4 Nov 2013: 8 of 21. [24] Thus, disentangling the effects of varying reflectioncoefficient and signal strength is not straightforward, espe-cially when tuning effects are important.

5 Oct 2013: Stable reconstructions in Hilbert spaces and the resolutionof the Gibbs phenomenon. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of

19 Oct 2013: Manuscript received 19 June 1998, in final form 24 March 1999).

19 Oct 2013: From M. Shapiro and S. Grnas (eds.), 1998: The Life Cycles of Extratropical Cyclones. Boston, Amer. Meteorol.Soc., preprint in press.Numerical Weather Prediction: a Vision of the Future, Updated Still FurtherMichael E. McIntyreCentre for Atmospheric

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

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

26 Jul 2013: dt 2. [4. 5 O (3). ], (24). 5. J. Phys.: Condens.

4 Oct 2013: n2π2 1. (24). On the other hand we had in a previous example the expression constructed from homo-geneous solutions:. ... ξ. (25). Now comparing eqs (24,25) and viewing ξ as a parameter and x as the independentvariable, we see that the equivalence of

3 Feb 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

26 Jul 2013: The first type of model, termed sublayer modeling, con-siders the dynamics of individual cilia, either theoretically ina simplified fashion,4,5 or numerically with all hydrodynamicinteractions.24,25 The study ... 1. Ln x0, t2. x0 tdx0. 24. For a given

4 Nov 2013: The elastic spreading law (5) thus implies. RðtÞ 0:40g. B. 5=24.

26 Jul 2013: we employ insteadthe full non-local SBT [24] to study the hydrodynamics ofthe superhelical swimmers. ... Þ. hþðh. (Þð%Þ. j Uþ(Vj=V. ðj U((Vj=VÞð%. Þ. Aedes. notoscriptus. 0.24.

26 Jul 2013: Other avenues of current active research in-clude the swimming dynamics of bodies in non-Newtonianfluid environments, such as the propulsion of spermatozoa inthe human female reproductive tract.24–29. ... studied spermatozoa of the seaurchin

26 Jul 2013: mental22 or locomotive processes.23,24. aDepartment of Physics, University of California San Diego, 9500 GilmanDrive, La Jolla, CA, 92093-0354.

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