Search

8 Jun 2013: 54. See SupplementaryInformation for more discussion of these tests.Model freshwater forcing.

26 Jul 2013: This. simple test illustrates the fundamental difference between the. propulsion of rigid chiral objects and flexible propellers.

26 Jul 2013: S hc. Ucu S, τ p De(u τ p GT τ p τ p G) (1 ζ )(G GT ). }= 0, (13). where S denotes the test function for τ p,

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

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

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: 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.

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

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).

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