Developing GPU-Enabled Scientific Librariesknepley/presentations/PresSimulaCBC2011.… ·...
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Developing GPU-Enabled Scientific Libraries
Matthew Knepley
Computation InstituteUniversity of Chicago
Department of Molecular Biology and PhysiologyRush University Medical Center
CBC Workshop on CBC Key TopicsSimula Research Laboratory
Oslo, Norway August 25–26, 2011
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Scientific Libraries
Outline
1 Scientific LibrariesWhat is PETSc?
2 Linear Systems
3 Assembly
4 Integration
5 Yet To be Done
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Scientific Libraries
Main Point
To be widely accepted,
GPU computing must betransparent to the user,
and reuse existinginfrastructure.
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Scientific Libraries
Main Point
To be widely accepted,
GPU computing must betransparent to the user,
and reuse existinginfrastructure.
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Scientific Libraries
Main Point
To be widely accepted,
GPU computing must betransparent to the user,
and reuse existinginfrastructure.
M. Knepley (UC) GPU CBC 4 / 85
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Scientific Libraries
Lessons from Clusters and MPPs
FailureParallelizing CompilersAutomatic program decomposition
SuccessMPI (Library Approach)PETSc (Parallel Linear Algebra)User provides only the mathematical description
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Scientific Libraries
Lessons from Clusters and MPPs
FailureParallelizing CompilersAutomatic program decomposition
SuccessMPI (Library Approach)PETSc (Parallel Linear Algebra)User provides only the mathematical description
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Scientific Libraries What is PETSc?
Outline
1 Scientific LibrariesWhat is PETSc?
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Scientific Libraries What is PETSc?
How did PETSc Originate?
PETSc was developed as a Platform forExperimentation
We want to experiment with differentModelsDiscretizationsSolversAlgorithms
which blur these boundaries
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Scientific Libraries What is PETSc?
The Role of PETSc
Developing parallel, nontrivial PDE solvers thatdeliver high performance is still difficult and re-quires months (or even years) of concentratedeffort.
PETSc is a toolkit that can ease these difficul-ties and reduce the development time, but it isnot a black-box PDE solver, nor a silver bullet.— Barry Smith
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Scientific Libraries What is PETSc?
Advice from Bill Gropp
You want to think about how you decompose your datastructures, how you think about them globally. [...] If youwere building a house, you’d start with a set of blueprintsthat give you a picture of what the whole house lookslike. You wouldn’t start with a bunch of tiles and say.“Well I’ll put this tile down on the ground, and then I’llfind a tile to go next to it.” But all too many people try tobuild their parallel programs by creating the smallestpossible tiles and then trying to have the structure oftheir code emerge from the chaos of all these littlepieces. You have to have an organizing principle ifyou’re going to survive making your code parallel.
(http://www.rce-cast.com/Podcast/rce-28-mpich2.html)
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Scientific Libraries What is PETSc?
What is PETSc?
A freely available and supported researchcode for the parallel solution of nonlinearalgebraic equations
FreeDownload from http://www.mcs.anl.gov/petscFree for everyone, including industrial users
SupportedHyperlinked manual, examples, and manual pages for all routinesHundreds of tutorial-style examplesSupport via email: [email protected]
Usable from C, C++, Fortran 77/90, Matlab, Julia, and Python
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Scientific Libraries What is PETSc?
What is PETSc?
Portable to any parallel system supporting MPI, including:Tightly coupled systems
Cray XT6, BG/Q, NVIDIA Fermi, K ComputerLoosely coupled systems, such as networks of workstations
IBM, Mac, iPad/iPhone, PCs running Linux or Windows
PETSc HistoryBegun September 1991Over 60,000 downloads since 1995 (version 2)Currently 400 per month
PETSc Funding and SupportDepartment of Energy
SciDAC, MICS Program, AMR Program, INL Reactor ProgramNational Science Foundation
CIG, CISE, Multidisciplinary Challenge Program
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Scientific Libraries What is PETSc?
The PETSc Team
Bill Gropp Barry Smith Satish Balay
Jed Brown Matt Knepley Lisandro Dalcin
Hong Zhang Mark Adams Toby IssacM. Knepley (UC) GPU CBC 12 / 85
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Scientific Libraries What is PETSc?
Who Uses PETSc?
Computational Scientists
Earth SciencePyLith (CIG)Underworld (Monash)Magma Dynamics (LDEO, Columbia, Oxford)
Subsurface Flow and Porous MediaSTOMP (DOE)PFLOTRAN (DOE)
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Scientific Libraries What is PETSc?
Who Uses PETSc?
Computational Scientists
CFDFiredrakeFluidityOpenFOAMfreeCFDOpenFVM
MicroMagneticsMagPar
FusionXGCBOUT++NIMROD
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Scientific Libraries What is PETSc?
Who Uses PETSc?
Algorithm Developers
Iterative methodsDeflated GMRESLGMRESQCGSpecEst
Preconditioning researchersPrometheus (Adams)ParPre (Eijkhout)FETI-DP (Klawonn and Rheinbach)
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Scientific Libraries What is PETSc?
Who Uses PETSc?
Algorithm Developers
Finite ElementslibMeshMOOSEPETSc-FEMDeal IIOOFEM
Other SolversFast Multipole Method (PetFMM)Radial Basis Function Interpolation (PetRBF)Eigensolvers (SLEPc)Optimization (TAO)
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Scientific Libraries What is PETSc?
What Can We Handle?
PETSc has run implicit problems with over 500 billion unknownsUNIC on BG/P and XT5PFLOTRAN for flow in porous media
PETSc has run on over 290,000 cores efficientlyUNIC on the IBM BG/P Jugene at JülichPFLOTRAN on the Cray XT5 Jaguar at ORNL
PETSc applications have run at 23% of peak (600 Teraflops)Jed Brown on NERSC EdisonHPGMG code
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Scientific Libraries What is PETSc?
What Can We Handle?
PETSc has run implicit problems with over 500 billion unknownsUNIC on BG/P and XT5PFLOTRAN for flow in porous media
PETSc has run on over 290,000 cores efficientlyUNIC on the IBM BG/P Jugene at JülichPFLOTRAN on the Cray XT5 Jaguar at ORNL
PETSc applications have run at 23% of peak (600 Teraflops)Jed Brown on NERSC EdisonHPGMG code
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Scientific Libraries What is PETSc?
What Can We Handle?
PETSc has run implicit problems with over 500 billion unknownsUNIC on BG/P and XT5PFLOTRAN for flow in porous media
PETSc has run on over 290,000 cores efficientlyUNIC on the IBM BG/P Jugene at JülichPFLOTRAN on the Cray XT5 Jaguar at ORNL
PETSc applications have run at 23% of peak (600 Teraflops)Jed Brown on NERSC EdisonHPGMG code
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Interface Questions
How should the user interact withmanycore systems?Through computational libraries
How should the user interact with the library?Strong, data structure-neutral API (Smith and Gropp, 1996)
How should the library interact withmanycore systems?
Existing library APIsCode generation (CUDA, OpenCL, PyCUDA)Custom multi-language extensions
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Scientific Libraries What is PETSc?
Performance Analysis
In order to understand and predict the performance of GPU code, weneed:
good models for the computation, which make it possible to evaluatethe efficiency of an implementation;
a flop rate, which tells us how well we are utilizing the hardware;
timing, which is what users care about;
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Linear Systems
Outline
1 Scientific Libraries
2 Linear Systems
3 Assembly
4 Integration
5 Yet To be Done
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Linear Systems
Performance ExpectationsLinear Systems
The Sparse Matrix-Vector product (SpMV)is limited by system memory bandwidth,
rather than by peak flop rate.
We expect bandwidth ratio speedup (3x–6x for most systems)
Memory movement is more important than minimizing flops
Kernel is a vectorized, segmented sum (Blelloch, Heroux, andZagha: CMU-CS-93-173)
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Linear Systems
Memory Bandwidth
All computations in this presentation are memory bandwidth limited.We have a bandwidth peak, the maximum flop rate achievable given abandwidth. This depends on β, the ratio of bytes transferred to flopsdone by the algorithm.
Processor BW (GB/s) Peak (GF/s) BW Peak∗ (GF/s)Core 2 Duo 4 34 1GeForce 9400M 21 54 5GTX 285 159 1062 40Tesla M2050 144 1030 36
∗Bandwidth peak is shown for β = 4
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Linear Systems
STREAM Benchmark
Simple benchmark program measuring sustainable memory bandwidth
Protoypical operation is Triad (WAXPY): w = y + αxMeasures the memory bandwidth bottleneck (much below peak)Datasets outstrip cache
Machine Peak (MF/s) Triad (MB/s) MF/MW Eq. MF/sMatt’s Laptop 1700 1122.4 12.1 93.5 (5.5%)Intel Core2 Quad 38400 5312.0 57.8 442.7 (1.2%)Tesla 1060C 984000 102000.0* 77.2 8500.0 (0.8%)
Table: Bandwidth limited machine performance
http://www.cs.virginia.edu/stream/
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Linear Systems
Analysis of Sparse Matvec (SpMV)
AssumptionsNo cache missesNo waits on memory references
Notationm Number of matrix rowsnz Number of nonzero matrix elementsV Number of vectors to multiply
We can look at bandwidth needed for peak performance(8 +
2V
)mnz
+6V
byte/flop (1)
or achieveable performance given a bandwith BWVnz
(8V + 2)m + 6nzBW Mflop/s (2)
Towards Realistic Performance Bounds for Implicit CFD Codes, Gropp,Kaushik, Keyes, and Smith.
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Linear Systems
Linear Algebra Interfaces
Strong interfaces mean:
Easy code interoperability (LAPACK, Trilinos)
Easy portability (GPU)
Seamless optimization
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Linear Systems
VECCUDA
Strategy: Define a new Vec implementation
Uses Thrust for data storage and operations on GPU
Supports full PETSc Vec interface
Inherits PETSc scalar type
Can be activated at runtime, -vec_type cuda
PETSc provides memory coherence mechanism
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Linear Systems
MATAIJCUDA
Also define new Mat implementations
Uses Cusp for data storage and operations on GPU
Supports full PETSc Mat interface, some ops on CPU
Can be activated at runtime, -mat_type aijcuda
Notice that parallel matvec necessitates off-GPU data transfer
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Linear Systems
Solvers
Solvers come for FreePreliminary Implementation of PETSc Using GPU,
Minden, Smith, Knepley, 2010
All linear algebra types work with solvers
Entire solve can take place on the GPUOnly communicate scalars back to CPU
GPU communication cost could be amortized over several solves
Preconditioners are a problemCusp has a promising AMG
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Linear Systems
ExampleDriven Cavity Velocity-Vorticity with Multigrid
ex50 -da_vec_type seqcusp-da_mat_type aijcusp -mat_no_inode # Setup types-da_grid_x 100 -da_grid_y 100 # Set grid size-pc_type none -pc_mg_levels 1 # Setup solver-preload off -cuda_synchronize # Setup run-log_summary
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Linear Systems
ExamplePFLOTRAN
Flow Solver32× 32× 32 grid
Routine Time (s) MFlops MFlops/sCPUKSPSolve 8.3167 4370 526MatMult 1.5031 769 512GPUKSPSolve 1.6382 4500 2745MatMult 0.3554 830 2337
P. Lichtner, G. Hammond,R. Mills, B. Phillip
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Linear Systems
Serial PerformanceNVIDIA GeForce 9400M
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Linear Systems
Serial PerformanceNVIDIA Tesla M2050
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Linear Systems
Serial PerformanceNVIDIA Tesla M2050
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Assembly
Outline
1 Scientific Libraries
2 Linear Systems
3 Assembly
4 Integration
5 Yet To be Done
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Assembly
Performance ExpectationsMatrix Assembly
Matrix Assembly, aggregation of inputs,is also limited by memory bandwidth,
rather than by peak flop rate.
We expect bandwidth ratio speedup (3x–6x for most systems)
Input for FEM is a set of element matrices
Kernel is dominated by sort (submission to TOMS)
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Assembly
Assembly Interface
A single new method is added:MatSetValuesBatch ( Mat J , Pe tsc In t Ne, Pe tsc In t Nl ,
Pe tsc In t *elemRows ,PetscScalar * elemMats )
Thus, a user just batches his input toachieve massive concurrency.
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input
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Assembly
Convenience Iterators
repeated_range < I n d e xA r r a y I t e r a t o r >rowInd ( elemRows . begin ( ) , elemRows . end ( ) , Nl ) ;
t i l ed_range < I nd e x A r r ay I t e r a to r >co l I nd ( elemRows . begin ( ) , elemRows . end ( ) , Nl , Nl ) ;
Nl = 3elemRows 0 1 3rowInd 0 0 0 | 1 1 1 | 3 3 3colInd 0 1 3 | 0 1 3 | 0 1 3
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column
1 Get permutation from (stably) sorting columns2 Gather rows with this permutation3 Get permutation from (stably) sorting rows4 Gather columns with this permutation5 Gather values with this permutation
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column
1 Get permutation from (stably) sorting columns2 Gather rows with this permutation3 Get permutation from (stably) sorting rows4 Gather columns with this permutation5 Gather values with this permutation
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Assembly
Multikey Sort
Initial input(1 0)(3 1)(0 0)(1 1)(3 3)(0 1)(0 3)(3 0)(1 3)
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Assembly
Multikey Sort
Number pairs Index(1 0) 0(3 1) 1(0 0) 2(1 1) 3(3 3) 4(0 1) 5(0 3) 6(3 0) 7(1 3) 8
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Assembly
Multikey Sort
After stable sort of columns Index(1 0) 0(0 0) 2(3 0) 7(3 1) 1(1 1) 3(0 1) 5(3 3) 4(0 3) 6(1 3) 8
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Assembly
Multikey Sort
After gather of rowsusing column permutation,and implicit renumbering
Index(1 0) 0(0 0) 1(3 0) 2(3 1) 3(1 1) 4(0 1) 5(3 3) 6(0 3) 7(1 3) 8
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Assembly
Multikey Sort
After stable sort of rows,and gather of columnsusing row permutation
Index(0 0) 1(0 1) 5(0 3) 7(1 0) 0(1 1) 4(1 3) 8(3 0) 2(3 1) 3(3 3) 6
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
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Assembly
Counting Unique Entries
Initial input (0 0)(0 1)(0 1)(0 3)(1 0)(1 1)(3 0)(3 0)(3 0)
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Assembly
Counting Unique Entries
Duplicate input (0 0) (0 0)(0 1) (0 1)(0 1) (0 1)(0 3) (0 3)(1 0) (1 0)(1 1) (1 1)(3 0) (3 0)(3 0) (3 0)(3 0) (3 0)
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Assembly
Counting Unique Entries
Shift new sequenceand truncate initial input
(0 0) (0 1)(0 1) (0 1)(0 1) (0 3)(0 3) (1 0)(1 0) (1 1)(1 1) (3 0)(3 0) (3 0)(3 0) (3 0)
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Assembly
Counting Unique Entries
“Multiply entries” usingnot-equals binary operator
(0 0) (0 1) =⇒ 1(0 1) (0 1) =⇒ 0(0 1) (0 3) =⇒ 1(0 3) (1 0) =⇒ 1(1 0) (1 1) =⇒ 1(1 1) (3 0) =⇒ 1(3 0) (3 0) =⇒ 0(3 0) (3 0) =⇒ 0
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Assembly
Counting Unique Entries
Reduction of entries plus 1gives number of uniqueentries
1(0 0) (0 1) =⇒ 1(0 1) (0 1) =⇒ 0(0 1) (0 3) =⇒ 1(0 3) (1 0) =⇒ 1(1 0) (1 1) =⇒ 1(1 1) (3 0) =⇒ 1(3 0) (3 0) =⇒ 0(3 0) (3 0) =⇒ 0
6
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
6 Allocate COO storage for final matrix7 Sum values with the same (i,j) index using reduce_by_key()
8 Convert to AIJ matrix9 Copy from GPU (if necessary)
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
6 Allocate COO storage for final matrix7 Sum values with the same (i,j) index using reduce_by_key()
8 Convert to AIJ matrix9 Copy from GPU (if necessary)
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
6 Allocate COO storage for final matrix7 Sum values with the same (i,j) index using reduce_by_key()
8 Convert to AIJ matrix9 Copy from GPU (if necessary)
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Assembly
Serial Assembly Steps
1 Copy elemRows and elemMat to device2 Allocate storage for intermediate COO matrix3 Use repeat&tile iterators to expand row input4 Sort COO matrix by row and column5 Compute number of unique (i,j) entries using inner_product()
6 Allocate COO storage for final matrix7 Sum values with the same (i,j) index using reduce_by_key()
8 Convert to AIJ matrix9 Copy from GPU (if necessary)
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes
1 Find number of off-process rows (serial)2 Map rows to processes (serial)3 Send number of rows to each process (collective)
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes
1 Find number of off-process rows (serial)2 Map rows to processes (serial)3 Send number of rows to each process (collective)
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes
1 Find number of off-process rows (serial)2 Map rows to processes (serial)3 Send number of rows to each process (collective)
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries
1 Partition into diagonal and off-diagonal&off-process usingpartition_copy ()
2 Partition again into off-diagonal and off-process usingstable_partition ()
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries
1 Partition into diagonal and off-diagonal&off-process usingpartition_copy ()
2 Partition again into off-diagonal and off-process usingstable_partition ()
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries
1 Partition into diagonal and off-diagonal&off-process usingpartition_copy ()
2 Partition again into off-diagonal and off-process usingstable_partition ()
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Assembly
Partitioning EntriesProcess owns rows [0, 3)
Initial input
(0,0) · · · (0,2) (0,3)...
. . .... (0,3)
(2,0) · · · (2,2) (0,3)(3,0) (3,1) (3,2) (3,3)
(3 0)(0 1)(3 3)(0 3)(0 0)(3 1)(1 3)(1 1)(1 0)
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Assembly
Partitioning EntriesProcess owns rows [0, 3)
Partition intodiagonal, andoff-diagonal &off-process entries
Diagonal
(0 0)(1 1)(0 1)(1 0)
Off-diagonalandOff-process
(3 1)(3 0)(1 3)(3 3)(0 3)
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Assembly
Partitioning EntriesProcess owns rows [0, 3)
Partition again intooff-diagonal andoff-process entries
Diagonal
(0 0)(1 1)(0 1)(1 0)
Off-diagonal(1 3)(0 3)
Off-process(3 1)(3 0)(3 3)
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries6 Send off-process entries7 Allocate storage for intermediate off-diagonal COO matrix8 Repartition entries into diagonal and off-diagonal using
partition_copy ()
9 Repeat serial assembly on both matrices
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries6 Send off-process entries7 Allocate storage for intermediate off-diagonal COO matrix8 Repartition entries into diagonal and off-diagonal using
partition_copy ()
9 Repeat serial assembly on both matrices
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries6 Send off-process entries7 Allocate storage for intermediate off-diagonal COO matrix8 Repartition entries into diagonal and off-diagonal using
partition_copy ()
9 Repeat serial assembly on both matrices
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries6 Send off-process entries7 Allocate storage for intermediate off-diagonal COO matrix8 Repartition entries into diagonal and off-diagonal using
partition_copy ()
9 Repeat serial assembly on both matrices
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Assembly
Parallel Assembly Steps
1 Copy elemRows and elemMat to device2 Use repeat&tile iterators to expand row input3 Communicate off-process entry sizes4 Allocate storage for intermediate diagonal COO matrix5 Partition entries6 Send off-process entries7 Allocate storage for intermediate off-diagonal COO matrix8 Repartition entries into diagonal and off-diagonal using
partition_copy ()
9 Repeat serial assembly on both matrices
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Assembly
Serial PerformanceNVIDIA GTX 285
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Integration
Outline
1 Scientific Libraries
2 Linear Systems
3 Assembly
4 IntegrationAnalytic FlexibilityComputational FlexibilityEfficiency
5 Yet To be Done
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Integration
What are the Benefits for current PDE Code?
Low Order FEM on GPUs
Analytic Flexibility
Computational Flexibility
Efficiency
http://www.bitbucket.org/aterrel/flamefem
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Integration
What are the Benefits for current PDE Code?
Low Order FEM on GPUs
Analytic Flexibility
Computational Flexibility
Efficiency
http://www.bitbucket.org/aterrel/flamefem
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Integration
What are the Benefits for current PDE Code?
Low Order FEM on GPUs
Analytic Flexibility
Computational Flexibility
Efficiency
http://www.bitbucket.org/aterrel/flamefem
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Integration
What are the Benefits for current PDE Code?
Low Order FEM on GPUs
Analytic Flexibility
Computational Flexibility
Efficiency
http://www.bitbucket.org/aterrel/flamefem
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Integration Analytic Flexibility
Outline
4 IntegrationAnalytic FlexibilityComputational FlexibilityEfficiency
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Integration Analytic Flexibility
Analytic FlexibilityLaplacian
∫T∇φi(x) · ∇φj(x)dx (3)
element = F in i teE lement ( ’ Lagrange ’ , te t rahedron , 1)v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )a = inner ( grad ( v ) , grad ( u ) ) * dx
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Integration Analytic Flexibility
Analytic FlexibilityLaplacian
∫T∇φi(x) · ∇φj(x)dx (3)
element = F in i teE lement ( ’ Lagrange ’ , te t rahedron , 1)v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )a = inner ( grad ( v ) , grad ( u ) ) * dx
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Integration Analytic Flexibility
Analytic FlexibilityLinear Elasticity
14
∫T
(∇~φi(x) +∇T ~φi(x)
):(∇~φj(x) +∇~φj(x)
)dx (4)
element = VectorElement ( ’ Lagrange ’ , te t rahedron , 1)v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )a = inner (sym( grad ( v ) ) , sym( grad ( u ) ) ) * dx
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Integration Analytic Flexibility
Analytic FlexibilityLinear Elasticity
14
∫T
(∇~φi(x) +∇T ~φi(x)
):(∇~φj(x) +∇~φj(x)
)dx (4)
element = VectorElement ( ’ Lagrange ’ , te t rahedron , 1)v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )a = inner (sym( grad ( v ) ) , sym( grad ( u ) ) ) * dx
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Integration Analytic Flexibility
Analytic FlexibilityFull Elasticity
14
∫T
(∇~φi(x) +∇T ~φi(x)
): C :
(∇~φj(x) +∇~φj(x)
)dx (5)
element = VectorElement ( ’ Lagrange ’ , te t rahedron , 1)cElement = TensorElement ( ’ Lagrange ’ , te t rahedron , 1 ,
( dim , dim , dim , dim ) )v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )C = C o e f f i c i e n t ( cElement )i , j , k , l = i nd i ces ( 4 )a = sym( grad ( v ) ) [ i , j ] *C[ i , j , k , l ] * sym( grad ( u ) ) [ k , l ] * dx
Currently broken in FEniCS release
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Integration Analytic Flexibility
Analytic FlexibilityFull Elasticity
14
∫T
(∇~φi(x) +∇T ~φi(x)
): C :
(∇~φj(x) +∇~φj(x)
)dx (5)
element = VectorElement ( ’ Lagrange ’ , te t rahedron , 1)cElement = TensorElement ( ’ Lagrange ’ , te t rahedron , 1 ,
( dim , dim , dim , dim ) )v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )C = C o e f f i c i e n t ( cElement )i , j , k , l = i nd i ces ( 4 )a = sym( grad ( v ) ) [ i , j ] *C[ i , j , k , l ] * sym( grad ( u ) ) [ k , l ] * dx
Currently broken in FEniCS release
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Integration Analytic Flexibility
Analytic FlexibilityFull Elasticity
14
∫T
(∇~φi(x) +∇T ~φi(x)
): C :
(∇~φj(x) +∇~φj(x)
)dx (5)
element = VectorElement ( ’ Lagrange ’ , te t rahedron , 1)cElement = TensorElement ( ’ Lagrange ’ , te t rahedron , 1 ,
( dim , dim , dim , dim ) )v = TestFunct ion ( element )u = T r i a l F u n c t i o n ( element )C = C o e f f i c i e n t ( cElement )i , j , k , l = i nd i ces ( 4 )a = sym( grad ( v ) ) [ i , j ] *C[ i , j , k , l ] * sym( grad ( u ) ) [ k , l ] * dx
Currently broken in FEniCS release
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Integration Analytic Flexibility
Form Decomposition
Element integrals are decomposed into analytic and geometric parts:
∫T ∇φi(x) · ∇φj(x)dx (6)
=∫T∂φi (x)∂xα
∂φj (x)∂xα dx (7)
=∫Tref
∂ξβ∂xα
∂φi (ξ)∂ξβ
∂ξγ∂xα
∂φj (ξ)∂ξγ|J|dx (8)
=∂ξβ∂xα
∂ξγ∂xα |J|
∫Tref
∂φi (ξ)∂ξβ
∂φj (ξ)∂ξγ
dx (9)
= Gβγ(T )K ijβγ (10)
Coefficients are also put into the geometric part.
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Integration Analytic Flexibility
Weak Form Processing
from f f c . ana l ys i s impor t analyze_formsfrom f f c . compi ler impor t compute_ir
parameters = f f c . defau l t_parameters ( )parameters [ ’ r ep resen ta t i on ’ ] = ’ tensor ’ana l ys i s = analyze_forms ( [ a , L ] , { } , parameters )i r = compute_ir ( ana lys is , parameters )
a_K = i r [ 2 ] [ 0 ] [ ’AK ’ ] [ 0 ] [ 0 ]a_G = i r [ 2 ] [ 0 ] [ ’AK ’ ] [ 0 ] [ 1 ]
K = a_K . A0 . astype (numpy . f l o a t 3 2 )G = a_G
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Integration Computational Flexibility
Outline
4 IntegrationAnalytic FlexibilityComputational FlexibilityEfficiency
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Integration Computational Flexibility
Computational Flexibility
We generate different computations on the fly,
and can changeElement Batch Size
Number of Concurrent Elements
Loop unrolling
Interleaving stores with computation
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Integration Computational Flexibility
Computational FlexibilityBasic Contraction
G K
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityBasic Contraction
G Kthread 0
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityBasic Contraction
G Kthread 0
thread 5
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityBasic Contraction
G Kthread 0
thread 5
thread 15
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityElement Batch Size
G0
G1
G2
G3
Kthread 0
thread 5
thread 15
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityElement Batch Size
G0
G1
G2
G3
K
thread 0
thread 5
thread 15
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityElement Batch Size
G0
G1
G2
G3
K
thre
ad0
thread 5
thread 15
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityElement Batch Size
G0
G1
G2
G3
K
thre
ad0
thread 5
thread 15
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityConcurrent Elements
G00
G01
G02
G03
G10
G11
G12
G13
Kthread 0
thread 5
thread 15
thread 16
thread 21
thre
ad31
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityConcurrent Elements
G00
G01
G02
G03
G10
G11
G12
G13
K
thread 0
thread 5
thread 15
thread 16thread 21
thre
ad31Figure: Tensor Contraction Gβγ(T )K ij
βγ
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Integration Computational Flexibility
Computational FlexibilityConcurrent Elements
G00
G01
G02
G03
G10
G11
G12
G13
Kth
read
0
thread 5
thread 15
thread 16thread 21
thread 31
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityConcurrent Elements
G00
G01
G02
G03
G10
G11
G12
G13
Kth
read
0
thread 5
thread 15
thread 16thread 21
thread 31
Figure: Tensor Contraction Gβγ(T )K ijβγ
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Integration Computational Flexibility
Computational FlexibilityLoop Unrolling
/ * G K c o n t r a c t i o n : u n r o l l = f u l l * /E [ 0 ] += G[ 0 ] * K [ 0 ] ;E [ 0 ] += G[ 1 ] * K [ 1 ] ;E [ 0 ] += G[ 2 ] * K [ 2 ] ;E [ 0 ] += G[ 3 ] * K [ 3 ] ;E [ 0 ] += G[ 4 ] * K [ 4 ] ;E [ 0 ] += G[ 5 ] * K [ 5 ] ;E [ 0 ] += G[ 6 ] * K [ 6 ] ;E [ 0 ] += G[ 7 ] * K [ 7 ] ;E [ 0 ] += G[ 8 ] * K [ 8 ] ;
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Integration Computational Flexibility
Computational FlexibilityLoop Unrolling
/ * G K c o n t r a c t i o n : u n r o l l = none * /f o r ( i n t b = 0; b < 1; ++b ) {
const i n t n = b * 1 ;f o r ( i n t alpha = 0; alpha < 3; ++alpha ) {
f o r ( i n t beta = 0; beta < 3; ++beta ) {E [ b ] += G[ n*9+ alpha *3+ beta ] * K [ alpha *3+ beta ] ;
}}
}
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Integration Computational Flexibility
Computational FlexibilityInterleaving stores
/ * G K c o n t r a c t i o n : u n r o l l = none * /f o r ( i n t b = 0; b < 4; ++b ) {
const i n t n = b * 1 ;f o r ( i n t alpha = 0; alpha < 3; ++alpha ) {
f o r ( i n t beta = 0; beta < 3; ++beta ) {E [ b ] += G[ n*9+ alpha *3+ beta ] * K [ alpha *3+ beta ] ;
}}
}/ * Store c o n t r a c t i o n r e s u l t s * /elemMat [ Eo f f se t + idx +0] = E [ 0 ] ;elemMat [ Eo f f se t + idx +16] = E [ 1 ] ;elemMat [ Eo f f se t + idx +32] = E [ 2 ] ;elemMat [ Eo f f se t + idx +48] = E [ 3 ] ;
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Integration Computational Flexibility
Computational FlexibilityInterleaving stores
n = 0;f o r ( i n t alpha = 0; alpha < 3; ++alpha ) {
f o r ( i n t beta = 0; beta < 3; ++beta ) {E += G[ n*9+ alpha *3+ beta ] * K [ alpha *3+ beta ] ;
}}/ * Store c o n t r a c t i o n r e s u l t * /elemMat [ Eo f f se t + idx +0] = E;n = 1; E = 0 . 0 ; / * con t rac t * /elemMat [ Eo f f se t + idx +16] = E;n = 2; E = 0 . 0 ; / * con t rac t * /elemMat [ Eo f f se t + idx +32] = E;n = 3; E = 0 . 0 ; / * con t rac t * /elemMat [ Eo f f se t + idx +48] = E;
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Integration Efficiency
Outline
4 IntegrationAnalytic FlexibilityComputational FlexibilityEfficiency
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Integration Efficiency
PerformanceInfluence of Element Batch Sizes
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Integration Efficiency
PerformanceInfluence of Element Batch Sizes
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Integration Efficiency
PerformanceInfluence of Code Structure
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Integration Efficiency
PerformanceInfluence of Code Structure
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Integration Efficiency
Performance
Price-Performance Comparison of CPU and GPU3D P1 Laplacian Integration
Model Price ($) GF/s MF/s$GTX285 390 90 231Core 2 Duo 300 2 6.6
∗ Jed Brown Optimization Engine
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Integration Efficiency
Performance
Price-Performance Comparison of CPU and GPU3D P1 Laplacian Integration
Model Price ($) GF/s MF/s$GTX285 390 90 231Core 2 Duo 300 12∗ 40
∗ Jed Brown Optimization Engine
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Yet To be Done
Outline
1 Scientific Libraries
2 Linear Systems
3 Assembly
4 Integration
5 Yet To be Done
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Yet To be Done
Competing Models
How should modern scientificcomputing be structured?
Current Model: PETSCSingle languageHand optimized3rd party librariesnew hardware
Alternative Model: PetCLAWMultiple language through PythonOptimization through code generation3rd party libaries through wrappersNew hardware through code generation
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Yet To be Done
Competing Models
How should modern scientificcomputing be structured?
Current Model: PETSCSingle languageHand optimized3rd party librariesnew hardware
Alternative Model: PetCLAWMultiple language through PythonOptimization through code generation3rd party libaries through wrappersNew hardware through code generation
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Yet To be Done
Competing Models
How should modern scientificcomputing be structured?
Current Model: PETSCSingle languageHand optimized3rd party librariesnew hardware
Alternative Model: PetCLAWMultiple language through PythonOptimization through code generation3rd party libaries through wrappersNew hardware through code generation
M. Knepley (UC) GPU CBC 83 / 85
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Yet To be Done
Competing Models
How should modern scientificcomputing be structured?
Current Model: PETSCSingle languageHand optimized3rd party librariesnew hardware
Alternative Model: PetCLAWMultiple language through PythonOptimization through code generation3rd party libaries through wrappersNew hardware through code generation
M. Knepley (UC) GPU CBC 83 / 85
![Page 128: Developing GPU-Enabled Scientific Librariesknepley/presentations/PresSimulaCBC2011.… · Developing GPU-Enabled Scientific Libraries Matthew Knepley Computation Institute University](https://reader034.fdocuments.us/reader034/viewer/2022051605/60161656c9b9cd632b0392bc/html5/thumbnails/128.jpg)
Yet To be Done
New Model for Scientific Software
Application
FFC/SyFieqn. definitionsympy symbolics
numpyda
tast
ruct
ures
petsc4py
solve
rs
PyCUDA
integration/assembly
PETScCUDA
OpenCL
Figure: Schematic for a generic scientific applicationM. Knepley (UC) GPU CBC 84 / 85
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Yet To be Done
What Do We Still Need?
Better integration of code generationMatch CUDA driver interface to CUDA runtime interface
Extend code generation to quadrature schemes
Kernel fusion in assembly
Better hierarchical parallelismLarger scale parallel GPU tests
Synchronization reduction in current algorithms
M. Knepley (UC) GPU CBC 85 / 85