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  2. J. Fluid Mech. (2002), vol. 458, pp. 283–301. c© ...

    www.itg.cam.ac.uk/people/heh/Paper171.pdf
    9 Mar 2004: Thus, formally, the head reacts to thedensity difference at the middle of its height, which is larger than zero (and henceinduces motion) even in the extreme case when ρc = ρb ... 2001). The objectives are (a) to test the ability of the numerical
  3. 30 Oct 2015: The model does, however, qualitativelycapture the observed behaviour. Using this value for E, the theoretical curve lies in the middle ofthe dimensionless data. ... This is expected because in the experiments of Ellison and Turner2 Res wasapproximately
  4. 16 Jul 2010: Thispossibility was also noted by Irvine (1980). To test thishypothesis further, Kerr & Tait (1985a) carried out aseries of experiments on crystal growth in a porousmedium using the Na2SO4-CuSO4-H2O ternarysystem. ... The hypothesis that wewished to test
  5. 20 Nov 2014: In order to test the predictiveability of our model in terms of sea-ice growth and salt fluxes, we compare its results with measurementsfrom laboratory experiments in section 3. ... 1997], not because they are necessarilybetter, but because they were
  6. J. Fluid Mech. (2001), vol. 447, pp. 1–29. c© ...

    www.itg.cam.ac.uk/people/heh/Paper164.pdf
    9 Mar 2004: Some test cases were also run with a direct solver for theblock tri-diagonal system. ... other runs with small C, as an additional test of the predictivepower of the numerical code and the SW approximation.
  7. flm1000488a

    www.itg.cam.ac.uk/people/heh/Paper224.pdf
    18 Jan 2011: 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 ... 1997, 19.3). The nonlinear diffusivity was estimated at the middle of the time step byfirst taking a
  8. 18 May 2017: This makes v2 negative.If ψ2 is positive, then the interface is concave in the middle and v2 is therefore positive. ... 3s2 7s) m[(1/4)(3s2 7s), s]. mψ [(1/4)(3s2 7s), s]. (5.25). To test the accuracy of the solution for ψ given by (5.25), it is
  9. jc001173 1..12

    www.itg.cam.ac.uk/people/grae/57.pdf
    26 Apr 2006: 4. Model Results. 4.1. Model Results for a Laboratory Experiment. [23] To test the model for the idealized diffusive case,governed by equations (1)–(5), we simulated the experi-ment ... All the other parameters werekept at the value indicated by the
  10. Multiple coexisting states of liquid rope coiling

    www.itg.cam.ac.uk/people/heh/Paper194.pdf
    17 May 2006: 1. 3. Inertio-gravitational regimeThe shapes of the curves shown in figure 5 differ significantly in the middle. ... To test whether these eigenfrequencies correspond to the multiple frequencies seen inthe full numerical solutions, we rescale the
  11. 14 Sep 2009: and (iii) the ability to test different, nonlinear constitutive laws for per-meability. ... There are important components of our simulations that are not validated by these two tests, including our treatment ofthe advection of solute and our success in

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