GPU acceleration of CaNS for massively-parallel direct numerical simulations of canonical fluid flows

Pedro Costa*, Everett Phillips, Luca Brandt, Massimiliano Fatica

*Corresponding author for this work

Research output: Contribution to journalArticleScientificpeer-review

19 Citations (Scopus)

Abstract

This work presents the GPU acceleration of the open-source code CaNS for very fast massively-parallel simulations of canonical fluid flows. The distinct feature of the many-CPU Navier–Stokes solver in CaNS is its fast direct solver for the second-order finite-difference Poisson equation, based on the method of eigenfunction expansions. The solver implements all the boundary conditions valid for this type of problems in a unified framework. Here, we extend the solver for GPU-accelerated clusters using CUDA Fortran. The porting makes extensive use of CUF kernels and has been greatly simplified by the unified memory feature of CUDA Fortran, which handles the data migration between host (CPU) and device (GPU) without defining new arrays in the source code. The overall implementation has been validated against benchmark data for turbulent channel flow and its performance assessed on a NVIDIA DGX-2 system (16 T V100 32Gb, connected with NVLink via NVSwitch). The wall-clock time per time step of the GPU-accelerated implementation is impressively small when compared to its CPU implementation on state-of-the-art many-CPU clusters, as long as the domain partitioning is sufficiently small that the data resides mostly on the GPUs. The implementation has been made freely available and open source under the terms of an MIT license.

Original languageEnglish
Pages (from-to)502-511
JournalComputers and Mathematics with Applications
Volume81
DOIs
Publication statusPublished - 2021
Externally publishedYes

Keywords

  • Computational fluid dynamics
  • Direct numerical simulation
  • Fast Poisson solver
  • GPU acceleration

Fingerprint

Dive into the research topics of 'GPU acceleration of CaNS for massively-parallel direct numerical simulations of canonical fluid flows'. Together they form a unique fingerprint.

Cite this