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5 Oct 2013: Using these values, in Figure 3 we plot the errors committed by the two methods for a varietyof different test functions.

5 Oct 2013: Generalized sampling and the stable and accuratereconstruction of piecewise analytic functions from their. Fourier coefficients. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre

26 Jul 2013: The numerical procedure was validated through conver-gence tests and by reproducing previous results for shearflow over sinusoidal surfaces.39 A large number of elements2N is needed when the sheets are

19 Oct 2013: This is a cumulative accuracy test, using the PV-conserving balanced model defined by a normal-mode-based PV inversion operatortogether with the single prognostic equation DQ/Dt = 0, for

4 Nov 2013: The effects of capillary forces on the axisymmetric propagation of two-phase, constant-flux gravity currents in porous mediaMadeleine J. Golding, Herbert E. Huppert, and Jerome A. Neufeld Citation: Phys. Fluids 25, 036602 (2013); doi:

5 Oct 2013: Using these values, in Figure 3 we plot the errors committed by the two methods for a varietyof different test functions.

4 Nov 2013: ln t =m1. ES+ m2 m3 ln(ES ) m4ES. (4.19). This enables us to extract the asymptotic nature of the solution and test the long-time limit (4.17) while

5 Oct 2013: Generalized sampling and the stable and accuratereconstruction of piecewise analytic functions from their. Fourier coefficients. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre

19 Oct 2013: May 31, 2010 Lecture Note Series, IMS, NUS — Review Vol. 9in x 6in lecturenotes˙190410. TRANSPORT AND MIXING OF ATMOSPHERIC. POLLUTANTS. Peter Haynes. Department of Applied Mathematics and Theoretical PhysicsUniversity of Cambridge. Wilberforce

5 Jun 2013: nuclear tests published in 1968. Using an instrumented aircraft, two ma-.

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: since its magnitude is O(a2 4). 6. Numerical ray tracingNumerical ray-tracing results are presented now that illustrate and test the.

5 Oct 2013: 3.5 Numerical ExamplesIn this section we will test the framework suggested in the previous section with the following frames: let{pk}kN denote the Legendre polynomials on [1, 1] and ... The assertion about K2m,r follows. 4.3 Numerical ExamplesIn this

5 Oct 2013: influence of the problem resolution.Naı̈ve simulations with standard, low-resolution test imagesmay very well lead to incorrect conclusions about the efficacyof compressed sensing as a tool for image reconstruction.

23 May 2013: 4] Davis, C.-I.: Numerical tests of the Fokas method for Helmholtz-type partial differential equations: Dirichlet to Neumann Maps,Masters Thesis, University of Colorado at Boulder (2008).

4 Nov 2013: 2007). Several small-scale demonstrationprojects have already commenced, pumping supercritical CO2 into brine-saturatedaquifers to test the viability of this technique. ... 5. Experimental analogueA series of analogue laboratory experiments were

26 Jul 2013: Recently, a study of light-activated colloidsreported the spontaneous surfing motion of reactive isotropic colloids lying on a solid surface,34 asystem which might be a potential candidate to test, at

26 Jul 2013: computed a linear controlstrategy, it is straightforward to test it on the nonlinearequation, and second, because the nonlinear modelbetter addresses the real problem of interest, that is,.

19 Oct 2013: Animportant test of this picture, after numerical renement, will be quantitativeconsistency between the predicted and observed interior angular velocities.Two quite dierent explanations for the near-uniform interior rotation of the

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

5 Oct 2013: 3.5 Numerical ExamplesIn this section we will test the framework suggested in the previous section with the following frames: let{pk}kN denote the Legendre polynomials on [1, 1] and ... The assertion about K2m,r follows. 4.3 Numerical ExamplesIn this

26 Jul 2013: test whether theideas put forward in this paper are valid.

5 Oct 2013: On optimal wavelet reconstructions from Fourier samples:. linearity and universality of the stable sampling rate. B. Adcocka, A. C. Hansenb,c, and C. Poonb. aDepartment of Mathematics, Purdue UniversitybDepartment of Applied Mathematics and

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

5 Oct 2013: On optimal wavelet reconstructions from Fourier samples:. linearity and universality of the stable sampling rate. B. Adcocka, A. C. Hansenb,c, and C. Poonb. aDepartment of Mathematics, Purdue UniversitybDepartment of Applied Mathematics and

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

5 Oct 2013: influence of the problem resolution.Naı̈ve simulations with standard, low-resolution test imagesmay very well lead to incorrect conclusions about the efficacyof compressed sensing as a tool for image reconstruction.

20 Dec 2013: By ”test body” we mean an uncharged object whose gravitational self-interactionis negligible, and whose size is much less than the length over which external fieldssuch as g vary. ... energy. Thus thefact that the motion of test bodies is consistent

24 Jun 2013: 4(b)]. To test whether m depends on the curvature oron the suspension size, we performed measurements withsuspensions diluted to 2=3 of the starting concentration.

27 Aug 2013: ResultsTo test the model and understand more about the regimes ofbehavior it possesses, we ran numerical integrations of the sys-tem starting from initial conditions of randomly perturbed totalfilament disorder (Materials ... Such an experiment would

4 Nov 2013: Each experiment was initiated by carefully releasing a constant flux of densesolution at the base of the narrow test cell.

26 Jul 2013: Both convergence tests. and comparison with known exact solutions were used to.

19 Oct 2013: The test flows (e.g., Fig. 1) are similar to those ex-tensively reported in Dritschel et al. ... Strin-gent convergence criteria are, however, essential if ouraccuracy tests are to be meaningful.

4 Nov 2013: 4. Experimental analogueA series of five experiments were performed in a Hele-Shaw cell as a test of. ... and a variety of λ. These experiments directly test the validity of both the functional form of the drainagevelocity and its inclusion within the

4 Oct 2013: 1)nbn/n converges by comparison test withM/n2 for a suitable constant M.

4 Nov 2013: The aim of this paper is twofold – (1) to compare the theory of gravity currents with experiments and simulations in homogeneous and heterogeneous porous media, and (2) to test the applicability

19 Oct 2013: measure of the geometry of a test tracer that is advected bythe flow (Haynes and Shuckburgh 2000a,b).

4 Nov 2013: J. Fluid Mech. (2013), vol. 719, pp. 551–586. c Cambridge University Press 2013 551doi:10.1017/jfm.2013.23. Convective shutdown in a porous medium athigh Rayleigh number. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1.

19 Oct 2013: J. Fluid Mech. (2005), vol. 534, pp. 67–95. c 2005 Cambridge University Pressdoi:10.1017/S0022112005004374 Printed in the United Kingdom. 67. Wave capture and wave–vortex duality. By OLIVER BÜHLER1 AND MICHAEL E. McINTYRE21Center for