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Routine Microsecond Molecular Dynamics Simulations with AMBER on GPUs. 1. Generalized Born
We present an implementation of generalized Born implicit solvent all-atom classical molecular dynamics (MD) within the AMBER program package that runs entirely on CUDA enabled NVIDIA graphics processing units (GPUs). We discuss the algorithms that are used to exploit the processing power of the GPU...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2012
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3348677/ https://www.ncbi.nlm.nih.gov/pubmed/22582031 http://dx.doi.org/10.1021/ct200909j |
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author | Götz, Andreas W. Williamson, Mark J. Xu, Dong Poole, Duncan Le Grand, Scott Walker, Ross C. |
author_facet | Götz, Andreas W. Williamson, Mark J. Xu, Dong Poole, Duncan Le Grand, Scott Walker, Ross C. |
author_sort | Götz, Andreas W. |
collection | PubMed |
description | We present an implementation of generalized Born implicit solvent all-atom classical molecular dynamics (MD) within the AMBER program package that runs entirely on CUDA enabled NVIDIA graphics processing units (GPUs). We discuss the algorithms that are used to exploit the processing power of the GPUs and show the performance that can be achieved in comparison to simulations on conventional CPU clusters. The implementation supports three different precision models in which the contributions to the forces are calculated in single precision floating point arithmetic but accumulated in double precision (SPDP), or everything is computed in single precision (SPSP) or double precision (DPDP). In addition to performance, we have focused on understanding the implications of the different precision models on the outcome of implicit solvent MD simulations. We show results for a range of tests including the accuracy of single point force evaluations and energy conservation as well as structural properties pertainining to protein dynamics. The numerical noise due to rounding errors within the SPSP precision model is sufficiently large to lead to an accumulation of errors which can result in unphysical trajectories for long time scale simulations. We recommend the use of the mixed-precision SPDP model since the numerical results obtained are comparable with those of the full double precision DPDP model and the reference double precision CPU implementation but at significantly reduced computational cost. Our implementation provides performance for GB simulations on a single desktop that is on par with, and in some cases exceeds, that of traditional supercomputers. |
format | Online Article Text |
id | pubmed-3348677 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2012 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-33486772012-05-09 Routine Microsecond Molecular Dynamics Simulations with AMBER on GPUs. 1. Generalized Born Götz, Andreas W. Williamson, Mark J. Xu, Dong Poole, Duncan Le Grand, Scott Walker, Ross C. J Chem Theory Comput We present an implementation of generalized Born implicit solvent all-atom classical molecular dynamics (MD) within the AMBER program package that runs entirely on CUDA enabled NVIDIA graphics processing units (GPUs). We discuss the algorithms that are used to exploit the processing power of the GPUs and show the performance that can be achieved in comparison to simulations on conventional CPU clusters. The implementation supports three different precision models in which the contributions to the forces are calculated in single precision floating point arithmetic but accumulated in double precision (SPDP), or everything is computed in single precision (SPSP) or double precision (DPDP). In addition to performance, we have focused on understanding the implications of the different precision models on the outcome of implicit solvent MD simulations. We show results for a range of tests including the accuracy of single point force evaluations and energy conservation as well as structural properties pertainining to protein dynamics. The numerical noise due to rounding errors within the SPSP precision model is sufficiently large to lead to an accumulation of errors which can result in unphysical trajectories for long time scale simulations. We recommend the use of the mixed-precision SPDP model since the numerical results obtained are comparable with those of the full double precision DPDP model and the reference double precision CPU implementation but at significantly reduced computational cost. Our implementation provides performance for GB simulations on a single desktop that is on par with, and in some cases exceeds, that of traditional supercomputers. American Chemical Society 2012-03-26 2012-05-08 /pmc/articles/PMC3348677/ /pubmed/22582031 http://dx.doi.org/10.1021/ct200909j Text en Copyright © 2012 American Chemical Society http://pubs.acs.org This is an open-access article distributed under the ACS AuthorChoice Terms & Conditions. Any use of this article, must conform to the terms of that license which are available at http://pubs.acs.org. |
spellingShingle | Götz, Andreas W. Williamson, Mark J. Xu, Dong Poole, Duncan Le Grand, Scott Walker, Ross C. Routine Microsecond Molecular Dynamics Simulations with AMBER on GPUs. 1. Generalized Born |
title | Routine Microsecond Molecular
Dynamics Simulations
with AMBER on GPUs. 1. Generalized Born |
title_full | Routine Microsecond Molecular
Dynamics Simulations
with AMBER on GPUs. 1. Generalized Born |
title_fullStr | Routine Microsecond Molecular
Dynamics Simulations
with AMBER on GPUs. 1. Generalized Born |
title_full_unstemmed | Routine Microsecond Molecular
Dynamics Simulations
with AMBER on GPUs. 1. Generalized Born |
title_short | Routine Microsecond Molecular
Dynamics Simulations
with AMBER on GPUs. 1. Generalized Born |
title_sort | routine microsecond molecular
dynamics simulations
with amber on gpus. 1. generalized born |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3348677/ https://www.ncbi.nlm.nih.gov/pubmed/22582031 http://dx.doi.org/10.1021/ct200909j |
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