Finite Element Discretization Library
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http://mfem.org
Version 3.3.3 (development)
===========================
More efficient non-conforming adaptive mesh refinement
------------------------------------------------------
- Significantly reduced MPI communication in the construction of the parallel
prolongation matrix in ParFiniteElementSpace, for much improved parallel
scaling of non-conforming AMR on hundreds of thousands of MPI tasks. The
memory footprint of the ParNCMesh class has also been reduced.
- In FiniteElementSpace, the fully assembled refinement matrix is now replaced
by default by a specialized refinement operator. The operator option is both
faster and more memory efficient than using the fully assembled matrix. The
old approach is still available and can be enabled, if needed, using the new
method FiniteElementSpace::SetUpdateOperatorType().
Discretization improvements
---------------------------
- Added classes for general block nonlinear finite element operators (deriving
from BlockNonlinearForm and ParBlockNonlinearForm) enabling solution of
nonlinear systems with multiple unknowns in different function spaces. Such
operators have assemble-based action and also support assembly of the gradient
operator to enable inversion with Newton iteration.
- Added variable order NURBS: for each space each knot vector in the mesh can
have a different order. The order information is now part of the finite
element space header in the NURBS mesh output, so NURBS meshes in the old
format need to be updated.
- Added symplectic integrators of orders 1-4 for systems of first order ODEs
derived from a Hamiltonian, see class SIASolver in linalg/ode.hpp.
- Inherit finite element classes from the new base class TensorBasisElement,
whenever the basis can be represented by a tensor product of 1D bases.
- Added support for elimination of boundary conditions in block matrices.
New and updated examples and miniapps
-------------------------------------
- Added a new serial and parallel example (ex19) that solves the quasi-static
incompressible hyperelastic equations. The example demonstrates the use of
block nonlinear forms as well as custom block preconditioners.
- Added a new electromagnetics miniapp, Maxwell, for simulating time-domain
electromagnetics phenomena as a coupled first order system of equations.
- A simple local refinement option has been added to the mesh-explorer miniapp
(menu option 'r', sub-option 'l') that selects elements for refinement based
on their spatial location - see the function 'region()' in the source file.
- Added a set of miniapps specifically focused on Isogeometric Analysis (IGA) on
NURBS meshes in the miniapps/nurbs directory. Currently the directory contains
variable order NURBS versions of examples 1, 1p and 11p.
- In the classes NonlinearForm and ParNonlinearForm, added support for
non-conforming AMR meshes; see also the "API changes" section.
- Added a new miniapp: miniapps/tools/load-dc.cpp, that can be used to visualize
fields saved via DataCollection classes.
- Example 10p with its SUNDIALS and PETSc versions have been updated to reflect
the change in the behavior of the method ParNonlinearForm::GetLocalGradient()
(see the "API changes" section) and now should work correctly on
non-conforming AMR meshes. Example 10 and its SUNDIALS version have also been
updated to support non-conforming ARM meshes.
Miscellaneous
-------------
- Documented project workflow and provided contribution guidelines in the new
top-level file, CONTRIBUTING.md.
- Added a new developer tool, config/sample-runs.sh, that extracts the sample
runs from all examples and miniapps and runs them. Optionally, it can save the
output from the execution to files, allowing comparison between different
versions and builds of the library.
- Add support for building a shared version of the MFEM library with GNU make.
- When building with the GnuTLS library, switch to using X.509 certificates for
secure socket authentication. Support for the previously used OpenPGP keys has
been deprecated in GnuTLS 3.5.x and removed in 3.6.0. For secure communication
with the visualization tool GLVis, a new set of certificates can be generated
using the latest version of the script 'glvis-keygen.sh' from GLVis.
- Upgraded MFEM to support Axom 0.2.8. Prior versions are no longer supported.
API changes
-----------
- Introduced a new enum, Matrix::DiagonalPolicy, that replaces the integer
parameters in many methods that perform elimination of rows and/or columns in
matrices. Some examples of such methods are:
* class SparseMatrix: EliminateRow(), EliminateCol(), EliminateRowCol(), ...
* class BilinearForm: EliminateEssentialBC(), EliminateVDofs(), ...
* class StaticCondensation: EliminateReducedTrueDofs()
* class BlockMatrix: EliminateRowCol()
Calling these methods with an explicitly given (integer) constants, will now
generate compilation errors, please use one of the new enum constants instead.
- Modified the virtual method AbstractSparseMatrix::EliminateZeroRows() and its
implementations in derived classes, to accept an optional 'threshold'
parameter, replacing previously hard-coded threshold values.
- In the classes NonlinearForm and ParNonlinearForm:
* The method GetLocalGradient() no longer imposes boundary conditions. The
motivation for the change is that, in the case of non-conforming AMR,
performing the elimination at the local level is incorrect - it must be
applied at the true-dof level.
* The method SetEssentialVDofs() is now deprecated.
Version 3.3.2, released on Nov 10, 2017
=======================================
High-order mesh optimization
----------------------------
- Added support for mesh optimization via node-movement based on the Target-
Matrix Optimization Paradigm (TMOP) developed by P.Knupp et al. A variety of
mesh quality metrics, with their first and second derivatives have been
implemented. The combination of targets & quality metrics is used to optimize
the physical node positions, i.e., they must be as close as possible to the
shape, size and/or alignment of their targets. The optimization of arbitrary
high-order meshes in 2D, 3D, serial and parallel is supported.
- The new Mesh Optimizer miniapp can be used to perform mesh optimization with
TMOP in serial and parallel versions. The miniapp also demonstrates the use of
nonlinear operators and their coupling to Newton methods for solving
minimization problems.
New and improved solvers and preconditioners
--------------------------------------------
- MFEM is now included in the xSDK project, the Extreme-scale Scientific
Software Development Kit, as of xSDK-0.3.0. Various changes were made to
comply with xSDK's community policies, https://xsdk.info/policies, including:
xSDK-specific options in CMake, support for user-provided MPI communicators,
runtime API for version number, and the ability to disable/redirect output.
For more details, see general/globals.hpp and in particular the mfem::err and
mfem::out streams replacing std::err and std::out respectively.
- Added (optional) support for the STRUMPACK parallel sparse direct solver and
preconditioner. STRUMPACK uses Hierarchically Semi-Separable (HSS) compression
in a fully algebraic manner, with interface similar to SuperLU_DIST. See
http://portal.nersc.gov/project/sparse/strumpack for more details.
- Added a block lower triangular preconditioner based (only) on the actions of
each block, see class BlockLowerTriangularPreconditioner.
- Added an optional operator in LOBPCG to projects vectors onto a desired
subspace (e.g. divergence-free). Other small changes in LOBPCG include the
ability to set the starting vectors and support for relative tolerance.
- The Newton solver supports an optional scaling factor, that can limit the
increment in the Newton step, see e.g. the Mesh Optimizer miniapp.
- Updated MFEM integration to support the new SUNDIALS 3.0.0 interface.
New and updated examples and miniapps
-------------------------------------
- Added a new serial and parallel example (ex18) that solves the transient Euler
equations on a periodic domain with explicit time integrators. In the process
extended the NonlinearForm class to allow for integrals over faces and
exchanging face-neighbor data in parallel.
- Added a new meshing miniapp, Shaper, that can be used to resolve complicated
material interfaces by mesh refinement, e.g. as a tool for initial mesh
generation from prescribed "material()" function. Both conforming and
non-conforming (isotropic and anisotropic) refinements are supported.
- Added a new meshing miniapp, Mesh Optimizer, that demonstrates the use of TMOP
for mesh optimization (serial and parallel version.)
- Added SUNDIALS version of Example 16/16p.
Discretization improvements
---------------------------
- Added a FindPoints method of the Mesh and ParMesh classes that returns the
elements that contain a given set of points, together with the coordinates of
the points in the reference space of the corresponding element. In parallel,
if a point is shared by multiple processors, only one of them will mark that
point as found. Note that the current implementation of this method is not
optimal and/or 100% reliable. See the mesh-explorer miniapp for an example.
- Added a new class InverseElementTransformation, that supports a number of
algorithms for inversion of general ElementTransformations. This class can be
used as a more flexible and extensible alternative to ElementTransformation's
TransformBack method. It is also used in the FindPoints methods as a tunable
and customizable inversion algorithm.
- Memory optimizations in the NCMesh class, which now uses 50% less memory than
before. The average cost of an element in a uniformly refined mesh (including
the refinement hierarchy, but excluding the temporary face_list and edge_list)
is now only about 290 bytes. This also makes the class faster.
- Added the ability to integrate delta functions on the right-hand side (by
sampling the test function at the center of the delta coefficient). Currently
this is supported in the DomainLFIntegrator, VectorDomainLFIntegrator and
VectorFEDomainLFIntegrator classes.
- Added five new linear interpolators in fem/bilininteg.cpp to compute products
of scalar and vector fields or products with arbitrary coefficients.
- Added matrix coefficient support to CurlCurlIntegrator.
- Extend the method NodalFiniteElement::Project for VectorCoefficient to work
with arbitrary number of vector components.
Miscellaneous
-------------
- Added a .gitignore file that ignores all files erased by "make distclean",
i.e. the files that can be generated from the source but we don't want to
track in the repository, as well as a few platform-specific files.
- Added Linux, Mac and Windows CI testing on GitHub with Travis CI and Appveyor.
- Added a new macro, MFEM_VERSION, defined as a single integer of the form
(major*100 + minor)*100 + patch. The convention is that an even number
(i.e. even patch number) denotes a "release" version, while an odd number
denotes a "development" version. See config/config.hpp.in.
- Added an option for building in parallel without a METIS dependency. This is
used for example the Laghos miniapp, https://github.com/CEED/Laghos.
- Modified the installation layout: all headers, except the master headers
(mfem.hpp and mfem-performance.hpp), are installed in /include/mfem;
the master headers are installed in both /include/mfem and in
/include. The mfem configuration and testing makefiles (config.mk and
test.mk) are installed in /share/mfem, instead of .
- Add three more options for MFEM_TIMER_TYPE.
- Support independent number of digits for cycle and rank in DataCollection.
- Converted Sidre usage from "asctoolkit" to "axom" namespace.
- Various small fixes and styling updates.
API changes
-----------
- The methods GetCoeff of VectorArrayCoefficient and MatrixArrayCoefficient now
return a pointer to Coefficient (instead of reference). Note that NULL pointer
is a valid entry for these two classes - it is treated as the zero function.
- When building with PETSc, the required PETSc version is now 3.8.0. Newer
versions may work too, as long as there are no interface changes in PETSc.
- The class GeometryRefiner now uses the enum in Quadrature1D for its type
specification. In particular, this will affect older versions of GLVis. A
simple upgrade to the latest version of GLVis should resolve this issue.
Version 3.3, released on Jan 28, 2017
=====================================
FEM <-> linear system interface for action-only linear operators
----------------------------------------------------------------
- Added a new class, ConstrainedOperator, which can impose essential boundary
conditions using only the action, Mult(), of a given square linear Operator.
- Added a FormLinearSystem + RecoverFEMSolution functionality for square linear
Operators that are available only through their action. This includes all
necessary transformations, such as: parallel assembly, conforming constraints
for non-conforming AMR and eliminating boundary conditions. (Hybridization and
static condensation are not supported.) See examples in miniapps/performance.
Matrix-free preconditioning and low-order-refined spaces
--------------------------------------------------------
- The HPC examples in miniapps/performance now support efficient preconditioning
in matrix-free mode based on applying a standard (e.g. AMG) preconditioner to
a sparsified version of the operator. The sparsification is obtained by
rediscretizing with a low-order refined spaces, currently at the high-order
degrees of freedom.
- New mesh constructors support the creation of low-order-refined version of a
given mesh, both in serial and in parallel. These are illustrated in the HPC
examples in miniapp/performance (option -pc lor), as well as in mesh-explorer
miniapp, which now supports Gauss-Lobatto refinement and uniform refinement,
both for any factor > 1.
Comprehensive PETSc and SUNDIALS interfaces
-------------------------------------------
- Added support for many linear and nonlinear solvers, preconditioners, time
integrators and other features from the PETSc suite (version 3.8 or higher of
the PETSc dev branch is required). The new features include:
* support for PETSc matrices in MATAIJ, MATIS, MATSHELL and MATNEST formats.
* PETSc linear solvers can take any mfem Operator and support user-defined
monitoring routines (see examples/petsc/ex1p).
* BDDC preconditioners for H1, H(curl) and H(div), including with static
condensation/hybridization, FieldSplit preconditioner for BlockOperators.
* PETSc non-linear solvers can take any mfem Operator that implements the
GetGradient() method.
* PETSc ODE solvers are supported for mfem's TimeDependentOperators.
The use of these features is illustrated in the new examples/petsc directory.
- Added a new class, OperarorHandle, that provides a common interface for
global, matrix-type operators to be used in bilinear forms, gradients of
nonlinear forms, static condensation, hybridization, etc.
The following backends are currently supported:
* HYPRE parallel sparse matrix (HYPRE_PARCSR)
* PETSC globally assembled parallel sparse matrix (PETSC_MATAIJ)
* PETSC parallel matrix assembled on each processor (PETSC_MATIS)
- Added support for the time integrators and non-linear solvers from the CVODE,
ARKODE and KINSOL libraries of the SUNDIALS suite (version 2.7 or higher of
SUNDIALS is required). The use of these features is illustrated in the new
examples/sundials directory.
Scalable parallel mesh support
------------------------------
- Introduced a new mesh format (v1.2) that can describe/recover MFEM parallel
meshes. This way, computations can start directly in parallel without serial
refinement and splitting. Non-conforming meshes are currently supported only
in serial.
General quadrature and nodal finite element basis types
-------------------------------------------------------
- Added support for different numerical quadrature schemes and finite element
basis points. Different basis points can be selected via optional integer
argument(s) to the finite element collection constructor of type BasisType:
* H1 elements can use GaussLobatto (default), Positive, or ClosedUniform;
* L2 elements can use GaussLegendre (default), GaussLobatto, Positive,
ClosedUniform, OpenUniform or OpenHalfUniform;
* RT can now use open basis that is GaussLegendre (default), GaussLobatto,
ClosedUniform, OpenUniform, or OpenHalfUniform, and closed basis that is
GaussLobatto (default) or ClosedUniform;
* ND elements can use the same BasisType's as RT elements.
- GaussLegendre, GaussLobatto, ClosedUniform, OpenUniform, and OpenHalfUniform
integration rules can be directly constructed with an optional parameter of
type Quadrature1D:
IntegrationRules gl(0, Quadrature1D::GaussLobatto);
const IntegrationRule *ir = gl(Geometry::SEGMENT, 5); // 4pt 1D rule
The global IntRules object continues to use GaussLegendre.
New integrators for common families of operators
------------------------------------------------
- Added MixedScalarIntegrator and 7 derived classes for integrating products of
two scalar basis functions and optional scalar coefficients.
- Added MixedVectorIntegrator and 16 derived classes for integrating the inner
product of two vector basis functions with optional scalar, vector, or matrix
coefficients.
- Added MixedScalarVectorIntegrator and 13 derived classes for integrating the
product of a scalar basis function with the inner product of a vector basis
function with a vector coefficient. In 2D the inner product can optionally be
replaced with a cross product.
- Added a new class DGElasticityIntegrator that supports a few types of DG
formulations for linear elasticity and a new linear form integrator,
DGElasticityDirichletLFIntegrator, that implements non-homogeneous BCs.
- Added support for DG spaces in class VectorBoundaryLFIntegrator.
- In classes BilinearForm and LinearForm, added support for boundary face
integrators applied to a subset of the boundary, see AddBdrFaceIntegrator.
New and updated examples and miniapps
-------------------------------------
- Sixteen new serial and parallel example codes that demonstrate:
* solution of a time-dependent nonlinear heat equation (Example 16/16p)
* DG formulations of static linear elasticity (Example 17/17p)
* the use of PETSc solvers and preconditioners (Examples 1p, 2p, 3p, 4p, 5p,
6p, 9p and 10p in examples/petsc)
* the use of SUNDIALS time integrators and nonlinear solvers (Examples 9/9p
and 10/10p in examples/sundials)
- The HPC examples in miniapps/performance now have a -mf/--matrix-free option
illustrating optimized "partial assembly" operator evaluation. This is now the
default in these examples, to switch to optimized matrix assembly instead use
the -asm/--assembly option.
- Added a new electromagnetic miniapp, Joule, illustrating the simulation of
transient magnetics and joule heating. This is a comprehensive miniapp that
uses finite element spaces and solvers for the whole de Rham sequence.
- Added a simple miniapp, display-basis, for displaying the various types
of finite element basis functions within single elements. This is part of
the new miniapps/tools directory.
- Rewrote the Volta and Tesla solver classes to avoid using linear algebra
objects when possible. This greatly simplifies the code, reduces memory
requirements, and eliminates unnecessary computation. It also fixed a bug
with divergence cleaning in the Tesla miniapp.
- Added an option to Example 9/9p to save a binary visualization file using the
Conduit mesh blueprint/hdf5 format.
Improved building options
-------------------------
- Added a new CMake build system, that can be used as an alternative to the GNU
make-based build system (e.g. for out-of-source building). For more details,
see the INSTALL file and the config/cmake directory.
- Added support for out-of-source builds with GNU make, see the INSTALL file.
Improved file output
--------------------
- Added on-the-fly compression of file streams input and output via gzstream,
see the MFEM_USE_GZSTREAM option.
- Added experimental support for an HDF5-based output file format following the
Conduit (https://github.com/LLNL/conduit) mesh blueprint specification for
visualization and/or restart capability. This functionality is aimed primarily
at user of LLNL's axom project (Sidre component) that run problems at extreme
scales. Users desiring a small scale binary format may want to look at the
gzstream functionality instead.
Miscellaneous
-------------
- Added optional support for software-based higher-precision arithmetic with
the MPFR library. When MFEM_USE_MPFR is enabled, the 1D quadrature rules will
be computed precisely, at least for rules with up to 65-points.
- Better support for METIS version 5 and above.
- Provide an informative backtrace in mfem_error based on the cross-platform
libunwind library (requires MFEM_USE_LIBUNWIND=YES).
- In class SparseMatrix, added methods PrintInfo and CheckFinite.
- GMRESSolver and MINRESSolver now support the same print levels as CGSolver.
- Added method MemoryUsage to the classes Stack and MemAlloc.
- Improved Doxygen formatting of code comments.
- Various other simplifications, extensions, and bugfixes in the code.
Version 3.2, released on Jun 30, 2016
=====================================
Dynamic AMR with parallel load balancing, derefinement of non-conforming meshes
-------------------------------------------------------------------------------
- Parallel non-conforming meshes can now be load balanced at any time by calling
ParMesh::Rebalance(). Elements of the mesh are redistributed in such a way
that each processor gets approximately the same number of elements (plus minus
one element). Partitioning is done by splitting a sequence of space-filling
(Hilbert) curves defined on the refinement octrees.
- Isotropically refined non-conforming meshes can now be derefined, both in
serial and in parallel, based on a per-element error measure and a
derefinement threshold. See the class ThresholdDerefiner.
- Following an arbitrary mesh change (uniform/general conforming/non-conforming
refinement, derefinement, load balancing), the FiniteElementSpace and
associated GridFunctions can be updated by interpolating or redistributing the
previous function values based on the new state of the mesh. (Internally this
is implemented through a transformation matrix that is constructed in the
FiniteElementSpace.) The user interface is quite simple:
pmesh.Rebalance(); // or GeneralRefinement, or GeneralDerefinement
fespace.Update(); // calculate a transformation matrix (by default)
x.Update(); // apply the transformation to the GridFunction
z.Update(); // apply it again
- New abstractions are available for error estimation and general mesh
operations such as refinement and derefinement. See the base classes
ErrorEstimator and MeshOperator and their descendants.
- The above features are illustrated in the new Example 15 (see also Example 6).
Tensor-based high-performance FEM operator assembly and evaluation
------------------------------------------------------------------
- Added support for high-performance, tensor-based efficient assembly and
evaluation of high-order operators.
- A number of new header files have been added to the fem/, linalg/ and mesh/
directories. They start with the prefix "t" to indicate the (heavy) use of C++
templating, similar to how the prefix "p" denotes "parallel". All the code for
the new HPC FE assembly/evaluation algorithms is fully implemented in these
header files. Note that the new interface is optional and only enabled if the
mfem-performance.hpp header is included instead of mfem.hpp. This is an
initial, reference implementation.
- Similarly to the serial-to-parallel (ex1.cpp-to-ex1p.cpp) transition, an
existing MFEM-based applications has to be transitioned to the new HPC
interface. This is illustrated in two new example codes which are the
high-performance versions of Example 1/1p. See miniapps/performance.
- The new interface reduces local operator assembly/evaluation to batched small
dense tensor contraction operations. For high performance, the sizes of these
contractions should be known at compile time, so the BilinearForm object needs
to have detailed knowledge about the mesh, the finite element space, the
quadrature rule and the integrator to be assembled. This required a new
interface, that supports a subset of the current (general) coefficients and
bilinear form integrators, including variable coefficients and mass and
diffusion integrators. It is possible to use the old and the new HPC interface
side-by-side, see the HPC version of Example 1/1p in miniapps/performance.
Advanced FEM on parallel non-conforming meshes
----------------------------------------------
- Added support for discontinuous Galerkin methods on parallel non-conforming
meshes, see Examples 9p and 14p.
- Added support for hybridization on parallel non-conforming meshes, see
Example 4p.
New and improved linear solvers
-------------------------------
- Added a wrapper for the real-valued, double precision solver in SuperLU_DIST
which is a sparse direct solver for distributed memory architectures. As such
it can only be enabled along with MFEM_USE_MPI. When MFEM is configured with
MFEM_USE_SUPERLU, one also needs to alter the version of METIS, since SuperLU
requires ParMETIS (which comes packaged with a serial version of METIS). See
http://http://crd-legacy.lbl.gov/~xiaoye/SuperLU for SuperLU_DIST details.
- Added a wrapper for the KLU solver in SuiteSparse see
http://faculty.cse.tamu.edu/davis/suitesparse.html for details of KLU.
If MFEM was configured with MFEM_USE_SUITESPARSE, one must now also link
against the klu and btf libraries in SuiteSparse, see config/defaults.mk.
New and updated examples and miniapps
-------------------------------------
- Four new serial and parallel example codes that demonstrate:
* high-performance finite element operator assembly/evaluation (Example 1/1p
in miniapps/performance)
* adaptive refinement, derefinement and load balancing (in parallel) on
non-conforming meshes (Example 15/15p)
- Examples 4p now supports hybridization on non-conforming meshes.
- Examples 9p and 14p now work on non-conforming meshes.
- Example 11p now has optional support for the SuperLU parallel direct solver.
- Added several new options and example runs in the Volta and Tesla miniapps,
including support for Halbach arrays of permanent magnets.
Miscellaneous
-------------
- Added "check" and "test" targets to the top-level makefile. The former does a
quick check by running Example 1/1p, while the latter does a more thorough
verification of the build by running all example codes and miniapps.
- Added support for 2D and 3D meshes generated by Gmsh (http://gmsh.info), both
in ASCII and binary formats.
- Added a reader for Cubit meshes in the Genesis (NetCDF) format. Currently
supported are linear and quadratic tet and hex meshes.
- Added support for boundary bilinear form integrators when using hybridization.
- Added support for Robin boundary conditions for DG in BoundaryMassIntegrator.
- Moved all reference element connectivity descriptions, such as element-edge,
element-face, etc. to the template class Geometry::Constants.
- Added support for secure socket communications in class socketstream based on
the GnuTLS library, see INSTALL for more details.
- Renamed config/user.mk.in to config/defaults.mk and moved all the default
build settings from the makefile there.
- Added configurable variables AR, ARFLAGS, and RANLIB in the build system. The
defaults for Mac OS X will suppress the "has no symbols" warnings.
- Various other simplifications, extensions, and bugfixes in the code.
API changes
-----------
- Changes in class Mesh
* Two-level state functionality was removed, including: UseTwoLevelState(int),
SetState(int), GetState(), GetNumFineElems(int), GetRefinementType(int),
GetFineElem(int, int) and GetFineElemTrans(int, int).
- Changes in class FiniteElementSpace
* BuildElementToDofTable() is now protected, and it is always called.
* GlobalRestrictionMatrix(FiniteElementSpace*, int) was removed, but the
prolongation operator can still be accessed via GetUpdateOperator() after
mesh refinement and a call to Update(true).
- Changes in methods related to non-conforming meshes and spaces
* The methods LinearForm::ConformingAssemble, BilinearForm::ConformingAssemble
and GridFunction::ConformingProlongate/ConformingProject are now hidden
inside (Par)BilinearForm::FormLinearSystem and RecoverFEMSolution.
* The conforming prolongation/restriction matrices can still be accessed via
FiniteElementSpace::GetConformingProlongation()/GetConformingRestriction().
- Changes in classes GridFunction and ParGridFunction
* Renamed Update((Par)FiniteElementSpace*, Vector&, int) to MakeRef.
* Renamed Update((Par)FiniteElementSpace*) to SetSpace.
Version 3.1, released on Feb 16, 2016
=====================================
Substantially improved non-conforming adaptive mesh refinement
--------------------------------------------------------------
- Added support for parallel non-conforming mesh refinement, including a new
example code with adaptive mesh refinement for the Laplace problem (Example
6p). Most of the example codes can now work on non-conforming meshes in serial
and in parallel.
- Added simple ZZ-type error estimators, including an anisotropic one in serial,
and one based on Raviart-Thomas flux projection in parallel, to the AMR
examples 6 and 6p. These seem to perform quite reasonably, even for
higher-order discretizations on 2D, 3D and surface meshes.
- The MFEM mesh format has a new version(1.1) that supports non-conforming
meshes. The format is an extension of 1.0 that includes a vertex_parents and
an optional coarse_elements section. See the example meshes amr-quad.mesh,
amr-hex.mesh and fichera-amr.mesh in the data/ directory.
- Added support for DG discretizations on non-conforming meshes in serial. See
the sample runs in Example 14.
- A new function, ParGridFunction::ParallelProject() directly returns a hypre
vector restricted to the true degrees of freedom (and supports non-conforming
meshes). In most cases, this should be preferred to the ParallelAverage()
function.
- When using non-conforming meshes, the essential boundary condition elimination
has to be applied at the end of the (parallel) assembly. Furthermore, in
serial, the bilinear form needs to call ConformingAssemble() after assembly
and the solution should call ConformingProlongate() after the solve (these are
not necessary in parallel). Note that these could also be handled
automatically by the new FEM <-> linear system interface, see below.
General finite element spaces and solvers on surfaces/skeletons
---------------------------------------------------------------
- Added support for arbitrary high-order finite element spaces on the mesh
skeleton (the faces, edges, and vertices between mesh elements) that are the
traces of the H1 and H(curl) spaces defined on the mesh. With the previously
existing H(div) trace space, the full de Rham sequence on the skeleton is now
supported.
- Updated integrators and discrete interpolators to work correctly for H(curl)
and H(div) spaces defined on surface meshes, or the mesh skeleton.
Hybridization, static condensation and a new FEM <-> linear system interface
----------------------------------------------------------------------------
- The BilinearForm/ParBilinearForm classes now support static condensation, as
well as hybridization (based on given constraint space and trace integrator).
These are illustrated in Examples 1-4.
- Added a new interface for transitioning between the finite element objects and
their corresponding linear algebra objects, which supports abstracts
transformations such as: parallel assembly, eliminating boundary conditions,
applying conforming constraints for non-conforming AMR, hybridization, static
condensation, back substitution, etc. Changed several of the example codes
accordingly.
New eigensolvers and improved solvers
-------------------------------------
- Added support for the scalable Locally Optimal Block Preconditioned Conjugate
Gradient (LOBPCG) eigenvalue solver and the Auxiliary-space Maxwell
Eigensolver (AME) from hypre.
- Added 3 new example codes to demonstrate the LOBPCG and AME applications to
the Laplace (Example 11p), Elasticity (Example 12p) and Maxwell (Example 13p)
eigenproblems.
- Updated the HypreAMS and HypreADS solvers to work for H(curl) and H(div)
problems defined on surface meshes, or the mesh skeleton.
- Added support for a discretization-enhanced version of hypre's BoomerAMG
designed specifically for linear elasticity problems, see Example 2p.
- The HypreAMS solver can now be used to solve singular curl-curl problems.
New and updated examples
------------------------
- Six new serial and parallel example codes that demonstrate:
* parallel conforming and non-conforming adaptive mesh refinement (Example 6p)
* hypre's LOBPCG eigensolver for the Laplace eigenproblem (Example 11p)
* hypre's LOBPCG eigensolver for the elasticity eigenproblem (Example 12p)
* hypre's AME eigensolver for the Maxwell eigenproblem (Example 13p)
* DG diffusion discretizations for the Laplace equation (Example 14/14p)
- Examples 1-4 now support static condensation, and Example 4/4p supports H(div)
hybridization, leading to much improved solve times. These examples also
illustrate the new interface for linear system assembly (see also Examples 6
and 7).
- Significantly improved the DPG preconditioner in Example 8p, which is now
scalable in parallel and uses the HypreADS solver to precondition the
interfacial block as an H(div) problem reduced to the mesh skeleton.
- Example 7/7p has a new option, -amr, showcasing simple local conforming and
non-conforming mesh refinements.
- Example 3/3p now works in both 2D and 3D.
New miniapps
------------
- Electromagnetic miniapps:
* Volta - simple electrostatics simulation code.
* Tesla - simple magnetostatics simulation code.
See also the README file in miniapps/electromagnetics.
- Meshing miniapps:
* Mobius Strip - generate various Mobius strip-like meshes.
* Klein Bottle - generate three types of Klein bottle surfaces.
* Mesh Explorer - visualize and manipulate meshes.
See also the README file in miniapps/meshing.
Miscellaneous
-------------
- Moved MFEM from Google Code to GitHub. New website: http://mfem.org.
- Formatted the code with Artistic Style, see the "make style" target.
- Added support for 64-bit integers in global size variables, enabling
simulations with >2B unknowns. (This requires that hypre is configured with
the --enable-bigint option.)
- Added optional support for the Gecko graph reordering library.
- Updated the implementation of some operations in DenseMatrix for better
auto-vectorization. Added a new class LUFactors that computes LU factorization
(with pivoting) and perform various operations with the factored data.
- Various other simplifications, extensions, and bugfixes in the code.
Version 3.0, released on Jan 26, 2015
=====================================
Improved documentation and build system
---------------------------------------
- Added interactive example documentation in examples/README.html. This should
be the starting point for new users interested in MFEM's features.
- New Doxygen-based code documentation. Due to its size, users are expected to
build this documentation themselves by typing make in the doc/ directory.
(Alternatively, the pre-build documentation can be browsed online).
- New build system, based on GNU make which consists of configuration and build
steps: "make config; make". The MFEM build options are exported, and can be
included in external makefiles. Library installation is also supported. See
"make help" and the INSTALL file for details.
- To build the examples use 'make' or 'make -j ' in the examples/ directory.
Based on the current MFEM configuration this will build the serial or the
parallel examples using the same config options as the library.
New and updated examples
------------------------
- Six new serial/parallel example codes that demonstrate:
* mixed pressure-velocity FEM for Darcy (Example 5)
* non-conforming adaptive mesh refinement for Laplace (Example 6)
* Laplace problem on a surface (Example 7)
* Discontinuous Petrov-Galerkin (DPG) for Laplace (Example 8)
* Discontinuous Galerkin (DG) time-dependent advection (Example 9)
* time-dependent implicit nonlinear elasticity (Example 10)
- Added command line options to all examples and modified several of the serial
ones to optionally use the serial direct solver UMFPACK.
- Simplified the elimination of Dirichlet boundary conditions in parallel.
- Grouped and documented the example code features in examples/README.html
Serial non-conforming adaptive mesh refinement
----------------------------------------------
- Added support for general, isotropic and anisotropic, local non-conforming
mesh refinement (using hanging nodes) in 2D and 3D, on quadrilateral,
triangular and hexahedral meshes. High-order curved and surface meshes are
also supported.
- The current implementation supports serial meshes (see example 6). Extension
to parallel meshes is in active development.
- The mesh is refined with Mesh::GeneralRefinement. The non-conforming mesh is
represented as a mesh that is "cut" along non-conforming edges and faces in
the internal NCMesh class. The only thing the user has to do to obtain a
continuous solution is to call BilinearForm::ConformingAssemble and
GridFunction::ConformingProlongate before and after solving the linear system.
The finite element space and grid functions are then updated with
FiniteElementSpace::UpdateAndInterpolate().
Time-dependent problems, non-linear operators and ODE integrators
-----------------------------------------------------------------
- Added new abstract base class TimeDependentOperator and a set of explicit
Runge-Kutta time integration classes in linalg/ode.?pp.
- Added classes for diagonally implicit Runge-Kutta (DIRK) time integrators
based on the ImplicitSolve() method of TimeDependentOperator.
- Extended all coefficient classes to be optionally time-dependent.
- Added classes for general nonlinear finite element operators (deriving from
NonlinearForm/ParNonlinearForm). Such operators have assemble-based action and
also support assembly of the gradient operator to enable inversion with Newton
iteration.
Discontinuous Galerkin and Discontinuous Petrov-Galerkin methods
----------------------------------------------------------------
- Added support Discontinuous Galerkin (DG) face integrators in parallel by
extending ParMesh with information for face-neighboring processors. Added DG
support in ParFiniteElementSpace, ParBilinearForm and ParGridFunction.
- Introduced a new class of integrators for forms defined on the faces of the
mesh (including interior and boundary faces), mainly intended for hybrid
methods like HDG and DPG that employ facet (numerical trace) spaces.
Block systems and rectangular operators
---------------------------------------
- Added classes BlockOperator, BlockVector and BlockMatrix for handling block
systems with different components (e.g., pressure and velocity).
- New abstract class AbstractSparseMatrix, between Matrix and SparseMatrix
- Modified class Operator to have two separate sizes: "height" and "width" for
the output and input sizes, respectively. The Size method was removed.
- For backward compatibility, the method Size is still present in the classes
DenseMatrix (returns width as before), SparseMatrix (returns height as
before), DenseMatrixInverse (square matrix) and BilinearForm (square matrix).
Linear and non-linear solvers
-----------------------------
- New abstract class Solver, with sub-classes for sparse smoothers, dense matrix
inverse, iterative solvers (Krylov methods and Newton) and the hypre solvers.
All Krylov methods were consolidated in linalg/solver.cpp and extended to work
in parallel.
- Added several new classes of solvers and smoothers:
* serial sparse direct solvers from the SuiteSparse library (UMFPACK)
* HypreSmoother, giving access to the parallel ParCSR smoothers in hypre
* polynomial smoothers: Chebyshev, Taubin and FIR
* stationary linear iteration (SLI)
* quadratic single linearly-constrained optimization problems with bounds
Miscellaneous
-------------
- Wrapped all classes/functions/objects in a namespace called "mfem".
- Automated the creation of quadrature rules to enable on-demand generation of
arbitrary order rules for all geometries 1D/2D/3D geometries.
- Added support for saving collections of grid functions in format suitable for
visualization with VisIt (visit.llnl.gov). See examples 5 and 9.
- Added support for 1D, surface and topologically periodic meshes, as well as a
simple inline mesh format. See the data/ directory for examples.
- Added support for serial mesh optimization using the Mesquite mesh quality
improvement toolkit (see mesh/mesquite.?pp and INSTALL for details).
- Made sure that MFEM can work in parallel with empty processors and with any
MPI communicator.
- Improved high-order Bernstein basis support.
- Support for high-resolution timers (e.g. POSIX clocks).
- Improved error messages with several macros, such as MFEM_ABORT, MFEM_VERIFY,
MFEM_ASSERT, MFEM_WARNING, etc.
- Improved portability for Windows (Visual Studio) and Mac OS X.
- Various simplifications, extensions, and bugfixes in the code.
Version 2.0, released on Nov 18, 2011
=====================================
Arbitrary order finite element spaces
-------------------------------------
- Added support for arbitrary high-order finite element spaces through the new
classes H1_FECollection, L2_FECollection, RT_FECollection and ND_FECollection.
These are based on a number of new FiniteElement sub-classes H1_*, L2_*, RT_*
and ND_* elements of arbitrary order on all types of reference elements.
- The classes implement H1-conforming, L2-discontinuous, H(div)-conforming
Raviart-Thomas and H(curl)-conforming Nedelec elements on triangular,
quadrilateral, tetrahedral and hexahedral meshes. The only restriction on the
order of the spaces is the availability of the required quadrature rules.
NURBS meshes and discretization spaces
--------------------------------------
- Added a collection of classes for serial and parallel meshes and
discretization spaces using Non-uniform rational B-splines (NURBS) basis
functions (files mesh/nurbs.?pp).
- The Mesh class supports the NURBS-specific refinement functions: KnotInsert
and DegreeElevate. Example NURBS meshes can found in the 'data' directory with
file names *-nurbs.mesh including an exact non-degenerate disc
(disc-nurbs.mesh) and exact non-degenerate ball (ball-nurbs.mesh).
- We can handle arbitrary NURBS or standard, non-NURBS, finite element spaces on
NURBS meshes. However, a NURBS finite element space requires an underlying
NURBS mesh. Refinement of parallel NURBS meshes is not supported yet.
Discrete gradient, curl, etc. matrices
--------------------------------------
- Added a new class, DiscreteLinearOperator, that facilitates the construction
of matrix representations for linear operators like gradient, curl, embedding,
projection, etc. The corresponding local "interpolators" are similar to
bilinear form integrators and derive from base class DiscreteInterpolator.
Current interpolators include GradientInterpolator, IdentityInterpolator,
CurlInterpolator and DivergenceInterpolator.
- Also available is a parallel version of DiscreteLinearOperator, which
assembles parallel topological matrices (such as the discrete gradient, curl,
etc.) in hypre's ParCSR format.
New integrators
---------------
- New linear (r.h.s.) integrator VectorFEBoundaryFluxLFIntegrator for
assembling (u, v.n) on the boundary for scalar u and v in an RT space.
- New bilinear integrator VectorFECurlIntegrator for assembling (curl u, v) for
u in a ND space and v in an RT space.
New and updated examples
------------------------
- Added a new serial/parallel Example code 4/4p, which solves a 2D or 3D H(Div)
diffusion problem using the Raviart-Thomas finite elements. In parallel, the
linear system is solved with the brand-new Auxiliary-space Divergence Solver
(ADS) in hypre.
- Modified Example 1 to use isoparametric discretization (use the FE space from
the mesh) including NURBS meshes and spaces. Updated Example 2 to support
arbitrary order spaces. Updated all examples to work with NURBS meshes and
spaces, as well as to not use projection onto discontinuous polynomial spaces
for visualization (this is now handled directly in GLVis when necessary).
- In all examples, switched to a uniform "solution" socket data type instead of
the various previous "*_gf_data" data types.
- In the parallel examples, switched to parallel mesh and solution output, as
well as to the new parallel socket format in place of PrintAsOne/SaveAsOne.
New hypre solvers
-----------------
- The parallel MFEM build now requires hypre 2.8.0b or newer.
- Extended HypreAMS and HypreADS to support (arbitrary) high-order ND/RT spaces,
by internally constructing the high-order ParDiscreteLinearOperator gradient,
curl and interpolation matrices. This makes the linear solve in Example 3p and
4p significantly faster than before. Extended the HypreAMS object to also work
for 2D H(div) problems.
Miscellaneous
-------------
- Added new class socketstream implementing two-way tcp/ip socket communications
in the framework of C++ streams. Added new class socketserver implementing
tcp/ip server functionality: listen on a given port for incoming connections,
and accept them by assigning the new connection to a socketstream. These new
classes are meant to replace the classes isockstream and osockstream. They
allow MFEM code to update the mesh and solution via a single socket connection
to a GLVis window.
- Added new Mesh and GridFunction constructors that combine multiple Mesh and
GridFunction objects into one object. These are used in GLVis to visualize
data saved in parallel. Removed obsolete code related to reading of parallel
disjoint meshes.
- Added more quadrature rules on triangles and tetrahedra.
- Basic experimental OpenMP support (disabled by default). When enabled, OpenMP
code is used for local matrix assembly, sparse matrix-vector product, and some
vector operations.
- Added support for METIS 5.0 (not the default, see INSTALL).
- Various simplifications, extensions, and bugfixes in the code.
Version 1.2, released on Apr 08, 2011
=====================================
Parallel MPI-based version of the library based on hypre
--------------------------------------------------------
- New MPI parallel version of the library based on the ParCSR parallel matrix
format from hypre and the metis graph partitioning library. This version
supports parallel local refinement and parallel curved meshes, as well as
several solvers from hypre.
New serial and parallel examples
--------------------------------
- Added a new example code describing an electromagnetic diffusion problem
discretized with lowest order Nedelec finite elements (Example 3).
- Added parallel versions of all examples codes (files ex1p.cpp, ex2p.cpp and
ex3p.cpp) based on hypre's BoomerAMG and AMS preconditioners.
Miscellaneous
-------------
- Added support for saving and reading linear and curved quadratic meshes in VTK
format. The format is automatically recognized when opening a mesh file, and
the boundary is reconstructed based on the actual domain boundary.
- The 'data' directory now contains a collection of various mesh files in the
MFEM and VTK formats, including curved meshes and the mesh files that were
previously in the 'examples' directory.
- Updated the default integration rule order for most of the linear form
integrators.
- Added support for cubic hex elements.
- Bugfixes in the face orientation of 3D RT0 elements and in the VectorFEDomain
linear form integrator.
- Various small fixes and styling updates.
Version 1.1, released on Sep 13, 2010
=====================================
New MFEM format for general meshes
----------------------------------
- New MFEM mesh v1.0 format with uniform structure for any dimension and support
for curved meshes including in 3D. Class Mesh will recognize and read the new
format (in addition to all previously used formats) and Mesh::Print uses the
new format by default. The old print function was renamed to Mesh::PrintXG.
New elasticity example
----------------------
- Added an example code for linear elasticity with (high-order) vector finite
elements (Example 2).
Miscellaneous
-------------
- Added Mesh::PrintVTK and GridFunction::SaveVTK methods for output in VTK
format.
- Implemented GeometryRefiner::Refine for CUBE and TETRAHEDRON geometries. This
allows for saving curved meshes in the VTK format.
- Added SConstruct file for mfem/examples.
- Various small fixes and styling updates.
Version 1.0, released on Jul 21, 2010
=====================================
- Uploaded to http://mfem.googlecode.com.
- Initial release.