| Parallel Domain Decomposition Solvers
for Large-Scale Reservoir Simulation
Contacts: Mary F.
Wheeler [email],
Marcelo Ramé [email],
Carol Woodward [email].
Domain decomposition
methods are a major area of contemporary researchin numerical
analysis of partial differential equations. They providerobust,
parallel and scalable preconditioned iterative methods for
thelarge-scale linear systems arising from discretization
of continuousproblems by finite elements, finite differences
or spectral methods.
In reservoir simulation,
large systems of linear or nonlinearequations have to be solved
at each time step, with one or more unknownsper grid block,
depending on the formulation of the discrete problem. These
linear systems or the linearization of nonlinear systems resultingfrom
Newton's method give rise to sparse, banded matrices amenable
tosolution by iterative methods. The spatial variability of
rock propertiesin a reservoir, as well as flow conditions
can yield mobility coefficientsjumping four to five orders
of magnitude over short distances. As aresult of this, the
associated algebraic system's matrices are highlyill-conditioned,
thus requiring the use of robust preconditioners fortheir
iterative solution.
Two such preconditioners
for the conjugate gradient method, which showthe required
robustness as well as excellent parallel scaling propertieswere
implemented for the three-dimensional, parallel simulatorRice-UTCHEM.
The capabilities of this code are presented elsewhere inthese
pages. The numerical discretization (IMPES) requires the solutionof
a linear system of pressure unknowns at each time step. All
othervariables of the model are updated explicitly. The block-centeredfinite-difference
discretization (equivalent to the lowest order mixedfinite
elements) gives rise to a pressure linear system which is
symmetricpositive definite.
Both the Balancing
Domain Decomposition (BDD) and the OverlappingAdditive Schwarz
(OAS) preconditioners for the conjugate gradient methodare
highlighted on this page. The BDD preconditioner is a nonoverlappingmethod
that solves for the interface unknowns between subdomains
asprimary unknowns (details of the method are given in [1]).
The OASpreconditioner is an overlapping preconditioner and
is implemented herewith minimal overlap, i.e., thickness =
1 grid-block (details are given in[2]). Both domain decomposition
preconditioners are compared against thediagonal or Jacobi
preconditioner in the figure shown. The matrix andvector of
right hand sides were generated by the parallel simulatorRiceUTCHEM
for a 3-D case with a mobility contrast of 3 orders ofmagnitude.
This is a problem of only modest complexity, both from thestandpoint
of the number of unknowns and the distribution of mobilitiesthroughout
the reservoir.

The figure shows,
on a log-log scale, the elapsed times required tosolve this
problem, on the Touchstone Delta (Intel massively-parallelprototype
machine at CalTech), using JCG, BDD-CG and OAS-CG. Decompositions
from 8 to 128 subdomains are shown on the graph. The solidblack
line, with a negative unit slope, indicates the ideal performance,i.e.,
doubling the number of processors reduces the time by a half.
BothDD methods solve this problem much faster than the Jacobi
preconditioner. Additionally, the poor scaling of the JCG
is evidenced by the slope of thecorresponding curve, which
is under unity in absolute value for all casestried. The DD
methods show much better scaling features up to the point(around
100 processors for this problem) where the subdomains become
tosmall and interprocessor communication starts to dominate
the elapsedtimes.
<<
Back to Software |