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13 Dec 2018: height both comparable with a wavelength. The tests (apart from the parallel code) wererun on a Pentium 4 3.2GHz with 1GB memory, under Linux.

31 Jan 2018: err. or. Dx2. Test code 3. 3. Variation with x of maximum error. ... I Comments on most lines. I Test for problems, halt with helpful message.

13 Dec 2018: We also test the algorithm with respect to measure-ment noise, by the addition of white noise to the scattereddata. ... For the linear profile problem, we also test the perfor-mance with respect to the noise data.

25 Oct 2018: The economic case – Dr Bhaskar Vira (Cambridge Conservation Research Institute and University Department of Geography)National government thinking – Rebecca Waite (DeFRA)Will there be enough water? –

19 Jan 2018: and similarly in three dimensions. Test error is O(x2) if piecewise linear bassis functions,and O(x4) if cubic splines. ... Capillary waves mean t <ρ/γx3/2. A good test is the vibration frequencies of an isolated drop.

1 Feb 2018: a. Time-stepping. No analytic solution to test. test code has designed accuracyO(t, x2). ... a. Time-stepping. No analytic solution to test test code has designed accuracyO(t, x2).

1 Feb 2018: Poisson problem. SOR. Test against theoretical solution: O(x2) error? 2.7 Vorticity evolution. ... a. Time-stepping. No analytic solution to test test code has designed accuracyO(t, x2).

31 Jan 2018: err. or. Dx2. Test code 3. 3. Variation with x of maximum error. ... I Comments on most lines. I Test for problems, halt with helpful message.

31 Dec 2018: No one really knew. what to do with his observation nor how to test the underlying atomic hypothesis.

25 Oct 2018: and similarly in three dimensions. Test error is O(x2) if piecewise linear bassis functions,and O(x4) if cubic splines. ... Capillary waves mean t <ρ/γx3/2. A good test is the vibration frequencies of an isolated drop.

28 Dec 2018: In order to test the code, the traditionalRayleigh-Bénard convection was solved for rigid-rigid boundary conditions, obtaining a neutralstability curve that compares very well to the standard result [30].

13 Dec 2018: Eds.), Physics of Estuaries and Coastal. Seas. White, T.E., 1995. Field tests of cross-shore sand transport models in oscilla-.

19 Sep 2018: Preprint typeset in JHEP style - PAPER VERSION Easter 2018. Variational Principles. Part 1A Mathematics Tripos. Prof. P.K. Townsend. DAMTP, CMS. Wilberforce Road, Cambridge CB3 0WA. E-mail: P.K.Townsend@damtp.cam.ac.uk. Abstract:. See schedules.

14 May 2018: 8 Non-Abelian Gauge Theory: Perturbative Quantization. We’re now ready to consider the quantum theory of Yang–Mills. In the first few sec-. tions, we’ll treat the path integral formally as an integral over infinite dimensional spaces,. without

28 Sep 2018: a. Time-stepping. No analytic solution to test. test code has designed accuracyO(t, x2). ... a. Time-stepping. No analytic solution to test test code has designed accuracyO(t, x2).

31 Jan 2018: 112. 23. 112. 0 112 0. ρ O(x4). Test. Analytic solution. ... Test. Analytic solution. ρ = 2π2 sin πx sin πy and φ = sin πx sin πy.

11 Jan 2018: PHYSICAL REVIEW FLUIDS 2, 123101 (2017). Bundling of elastic filaments induced by hydrodynamic interactions. Yi Man,1, William Page,2 Robert J. Poole,2 and Eric Lauga1,†1Department of Applied Mathematics and Theoretical Physics, University of

13 Dec 2018: This provides a test of the numerical solution for a given rough surface and allows the separation of the deter- ministic and stochastic components. ... Most usefully here, (25) provides a simple analytical test of the numerical solution for slightly

11 Oct 2018: and b = 1. Despite their apparent simplicity, linear programs have applications in many areas of appliedsciences, engineering and economics.

22 Jan 2018: Show that. P(D)[ϕψ] =|α|N. 1. α!Dα(ϕ)P (α)(D)(ψ). for all test functions ψ,ϕ D(Rn). ... It’s currently an open (and difficult). problem to show that a similar pointwise limit exists when the test function belongs to some Sobolev space Hs(Rn)