Comparison of simulations with both methods did not show noticeable differences. In this section, the performance of the embedded influx methods are illustrated with simulations of two numerical codes. One

code is a spectral implementation of the equations with exact dispersion. Results of simulations will be shown that are obtained with AB-models Anti-infection Compound Library purchase that have exact linear dispersion and are accurate up to and including second order terms; see van Groesen and Andonowati (2007), van Groesen et al. (2010), and van Groesen and van der Kroon (2012) for the 1D and She Liam and van Groesen (2010) for the 2D model. The other code is based on the Variational Boussinesq Model which has approximate dispersion as described in Section 2; see Klopman et al. (2010), Lakhturov et al. (2012), and Adytia and van Groesen (2012). To use the embedded influxing method in the FE implementation of this

Model, the source functions have to be constructed using the dispersion relation of the VBM itself; after transformation to physical space, the sources have to be discretized in the FE setting. For a case of strong nonlinear wave focusing, simulations with embedded point generation in the nonlinear AB equation selleck screening library are compared with experiments. The measurements were done at MARIN hydrodynamic laboratory (Maritime Research Institute Netherlands), case 109001. In a long tank with depth of 1m, the time signal of the measured surface elevation at one position, say at x  =0, is taken as the influx

signal, and measurements at two other positions x=19.2m and x=20.8m are used for comparison. The influxed signal consists of short waves followed by longer waves that have faster speed. The broad spectrum, and the strong focusing effect (with more than threefold amplitude amplification compared to the maximal influx amplitudes) make this a suitable test for the influx performance. The plots of the influx signal, and the modified signal that is used in the source term, are shown side by side in the first row of Fig. 7, with the Nintedanib supplier spectra of the two signals below it. Notice that the modified signal has higher amplitude and spectrum because of the multiplication with the group velocity as in expression (10). The comparison of results of the numerical simulation with the measurements is shown in Fig. 8 at two positions, one close-by and the other at almost the exact position of focusing. This figure shows that the focusing phenomenon, longer waves catch up with shorter waves and interfere constructively at the focusing point, is not only qualitatively but also quantitatively well-captured by the simulation. To illustrate influxing of oblique plane waves, an example is considered of oblique wave interaction in MARIN measurements in a wide tank of 5m depth for 300 s. One wave is influxed from the y  -axis for y∈[10,27]y∈[10,27] parallel to the x  -axis and has a period of 1.