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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.

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.

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: 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)

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

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

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: 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: 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).

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

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).

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

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

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: 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

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.

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

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