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Fig. 10

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Density rendering of the Kelvin-Helmholtz instability at t=2 (left column) and t=4 (right column) for an initial density contrast of ∆ρ = 2 (top panels) and ∆ρ = 8 (bottom panels) with the GDSPH 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 at a given Nsmooth and the popular Wendland C2 and C4 kernels. We observed a clear improvement in the optimized kernel, reproducing a similar behavior of the C4 kernel at double the neighbor count (Nsmooth). For the high density contrast ∆ρ = 8, there are only minor differences between the different kernels at Nsmooth = 128. These can be compared to the higher resolution cases given in Appendix A.

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