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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