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Fig. 11

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Density rendering of the Kelvin-Helmholtz instability at t = 4 for Nsmooth = 32 with the ISPH method. The X and Y axes have a length of one. Here one can see a comparison in the development of the instability between the optimized kernel (OI, 32) and the popular Wendland C2 and C4 kernels. We have selected three cases where discernible differences can be seen (nx = 128, ∆ρ = 2; nx = 64, ∆ρ = 2; nx = 128, ∆ρ = 8). For the ∆ρ = 2 cases we observed that the C2 and C4 kernels exhibit more angular momentum errors (inherent to ISPH) compared to the OI,32 kernel, where the inner stream becomes significantly twisted, deviating from the high resolution and high Nsmooth results (see Appendix A). For the high density case nx = 128, ∆ρ = 8, we observed that C4 is unable to generate the same vortex structure in the upper plane of the stream and exhibit some asymmetry around the plane.

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