Abstract

We present a new hydrodynamical code GPUPEGAS 2.0 for 3D simulation of astrophysical flows using the GPUs. This code is an extension of GPUPEGAS code developed in 2014 for simulation of interacting galaxies. GPUPEGAS 2.0 is based on the Authors’ numerical method of high order of accuracy for smooth solutions with small dissipation of the solution in discontinuities. The high order of accuracy and small dissipation are achieved by using the piecewise-linear representation of the physical variables in each dimension. The Rusanov flux allows one to simply vectorize the solution of the Riemann problem. The code was implemented for the cluster supercomputers NKS-30T (Siberian Supercomputer Center, SB RAS) and Uran (Institute of Mathematics and Mechanics, UrB RAS) using the hybrid MPI+CUDA technology. To avoid the compute capability-specific implementations of reduction routines, the Thrust library was used. The optimal parameters for kernel function were found for the three-dimensional computation grid. The Sedov point blast problem was used as a main test one. The numerical experiment was performed to simulate the hydrodynamics of the type II supernova explosion for the grid size of 2563. A set of experiments was performed to study performance and scalability of the developed code. The performance of 25 GFLOPS was achieved using a single Tesla M2090 GPU. The speedup of 3 times was achieved using a node with 4 GPUs. By using 16 GPUs, 70% scalability was achieved.

Highlights

  • Studying the hydrodynamics of the supernova explosions is an important astrophysical problem

  • We present a new code GPUPEGAS 2.0 for 3D simulation of astrophysical flows using the GPUs

  • The conservative and primitive variables are defined at the centers of cells

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Summary

Introduction

Studying the hydrodynamics of the supernova explosions is an important astrophysical problem. We present a new code GPUPEGAS 2.0 for 3D simulation of astrophysical flows using the GPUs. The code is based on the efficient piecewise-parabolic method on the local stencil [3, 4], which was successfully applied to a number of astrophysical problems [5, 6]. Where F (U ) is the flux vector of the conservative variables, Q is the right part vector describing the work of the gravitational forces.

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