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Cactus and Solving Einsteins Equations

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Title: Cactus and Solving Einsteins Equations


1
Cactus and Solving Einsteins Equations
  • Edward Wang
  • 2002.04.09
  • Yfwang_at_mail.ustc.edu.cn

2
Episode oneWhat is cactus?
http//www.cactus.org
3
Description
  • Cactus is an open source problem solving
    environment designed for scientists and
    engineers. Its modular structure easily enables
    parallel computation across different
    architectures and collaborative code development
    between different groups. Cactus originated in
    the academic research community, where it was
    developed and used over many years by a large
    international collaboration of physicists and
    computational scientists.

4
  • The name Cactus comes from the design of a
    central core (or "flesh") which connects to
    application modules (or "thorns") through an
    extensible interface. Thorns can implement custom
    developed scientific or engineering applications,
    such as computational fluid dynamics. Other
    thorns from a standard computational toolkit
    provide a range of computational capabilities,
    such as parallel I/O, data distribution, or
    checkpointing.

5
  • Cactus runs on many architectures.
    Applications, developed on standard workstations
    or laptops, can be seamlessly run on clusters or
    supercomputers. Cactus provides easy access to
    many cutting edge software technologies being
    developed in the academic research community,
    including the Globus Metacomputing Toolkit, HDF5
    parallel file I/O, the PETSc scientific library,
    adaptive mesh refinement, web interfaces, and
    advanced visualization tools.

6
http//www.globus.org/default.asp The Globus
Project is developing fundamental technologies
needed to build computational grids.
http//hdf.ncsa.uiuc.edu/HDF5/ HDF5 is a library
and file format for storing scientific data.
http//www-fp.mcs.anl.gov/petsc/ PETSc is a suite
of data structures and routines for the scalable
(parallel) solution of scientific applications
modeled by partial differential equations.
  • PETSc

7
Features
  • Highly Portable
  • Supported on most architectures
  • Sophisticated make system
  • Powerful Application Programming Interface
  • User modules (thorns) plug-into compact core
    (flesh)
  • Configurable interfaces, schedules and parameters

8
  • Advanced Computational Toolkit
  • Accessible MPI-based parallelism for finite
    difference grids
  • Access to a variety of supercomputing
    architectures and clusters
  • Several parallel I/O layers
  • Fixed and Adaptive mesh refinement under
    development
  • Elliptic solvers ?
  • Parallel interpolators and reductions ?
  • Metacomputing and distributed computing

9
  • Collaborative Development
  • Interactive monitoring, steering and
    visualization
  • Enables sharing code base.
  • TestSuite checking technology
  • Visualization tools
  • Exhaustive Numerical Relativity and Astrophysical
    Applications
  • Black Hole coalescence
  • Neutron star collisions
  • Other cataclysms

10
Applications
  • If your only goal is to implement a
    simulation of a 1D wave equation, you probably
    don't want to use Cactus. You should consider
    using Cactus if you need to perform any of the
    following tasks - now or in future
  • perform parallel programming in an easy but
    powerful manner using the language of your
    choice F77, F90, C, C.
  • run on a wide range of architectures and
    operating systems.
  • develop your code on the most convenient machine
    available, for example your workstation or laptop
    ...

11
  • and simply move your code to a supercomputer
    (like a Cray T3E or Origin) to go into production
    right away!
  • engage in high performance cluster computing or
  • get first parallel experience by turning your
    networked PC pool into a computing cluster.
  • work with collaborators on the same code and
    avoid having your programs fragmented.
  • make use of the latest software technology e.g.
    take advantage of research groups that spend
    their time thinking about the fastest way to
    bring simulation data to disk or how to visualize
    it while the code is running.

12
Supported Architectures
  •  Intel IA32 Linux
  • IBM SP
  • SGI 32 bit
  • Intel IA32 Windows NT
  • Cray T3E
  • SGI 64 bit
  • Intel IA32 Windows 2000
  • Intel IA64 Linux
  • Compaq Alpha
  • Sun Sparc
  • Hitachi SR8000-F1
  • MacOS X
  • Fujitsu(Beta 11) 

13
  • Cactus uses the cygwin package to provide a
    unix-like environment in windows os.

cvgwin
14
Associated Packages
  • MPI
  • LAM Version 6.5.4 and earlier
  • MPICH Version 1.2.2.1 and earlier
  • MPICH-G2
  • HDF5
  • Version 1.4 and 1.2

15
The Computational Toolkit
  • Cactus is architectured to consist of modules
    (we call them thorns) which plug into a core code
    (we call it the flesh) which contains the APIs
    and infrastructure to glue the thorns together.
  • The flesh on it's own doesn't actually do
    anything. The thorns contain all the real
    activity, and can usually be divided into
    application thorns (typically written by
    scientists, solving problems in physics,
    astrophysics, engineering, etc) and
    infrastructure thorns (typically written by
    computational scientists, providing IO,
    interpolations, drivers, elliptic solvers etc).
    We group thorns together into arrangements,
    depending on their functionality and
    applicability.

16
  • Drivers
  • Boundary Conditions
  • Coordinate Systems
  • Output Methods
  • Interpolators and Reduction Operators
  • Elliptic Solvers
  • Utilities

17
(No Transcript)
18
Live Demos
  • WaveToy DemoOur standard demonstration, see the
    description page for an explanation and how to
    run this yourself.
  • Cactus WormOur prototype dynamic Grid computing
    example ... this is being developed to add new
    features and fault tolerance ... please be
    understanding if it is down!

19
E-Grid and Cactus
  • The Cactus Team are closely involved with the
    activities of the European Grid Forum, in
    particular with the Working Group for Testbeds,
    which is headed by Ed Seidel. Cactus is being
    used by members of the E-Grid, along with the
    distributed computing toolkit Globus as an
    initial test application in a number of
    institutions.

20
  • Through work with the EGrid Consortium, Cactus
    will benefitfrom the development of
  • Access to a Europe wide Grid-TestBed, joining
    computing resources at over ten institutions.
  • More stable and secure methods of streaming data
    between simulation and various visualisation
    clients
  • Development of procedures and thorns for
    automatic migrating Cactus jobs
  • Ability to read streamed data into Cactus, e.g.
    checkpoint files
  • Ability to stream checkpoint files from Cactus
  • Increasing expertise in performing distributed
    runs

21
E-Grid TestBed
  • The E-Grid TestBed comprises a varied set of
    computational resources which was set up for
    demonstrations at SC2000 in Dallas, and provides
    a common and supported grid infrastructure with
    each site implementing
  • Globus 1.1.4
  • gsiftpd
  • gsisshd (using port 2222)
  • MPICH-G2 (MPICH 1.2.1 with Globus device)
  • HDF5 1.3.30 or above
  • GRIS reporting to TestBed GIIS
  • Cactus 4.0 Beta 9

22
Episode TwoSolving Einsteins Equations
http//www.computer.org/computer /articles/einstei
n_1299_1.htm
23
Einsteins Equations
  • Globally distributed scientific teams, linked
    to the most powerful supercomputers, are running
    visual simulations of Einsteins equations on the
    gravitational effects of colliding black holes.

24
  • In 1916, Albert Einstein published his
    famous general theory of relativity, which
    contains the rules of gravity and provides the
    basis for modern theories of astrophysics and
    cosmology. It describes phenomena on all scales
    in the universe, from compact objects such as
    black holes, neutron stars, and supernovae to
    large-scale structure formation such as that
    involved in creating the distribution of clusters
    of galaxies. For many years, physicists,
    astrophysicists, and mathematicians have striven
    to develop techniques for unlocking the secrets
    contained in Einsteins theory of gravity more
    recently, computational-science research groups
    have added their expertise to the endeavor.

25
  • Those who study these objects face a daunting
    challenge The equations are among the most
    complicated seen in mathematical physics.
    Together, they form a set of 10 coupled,
    nonlinear, hyperbolic-elliptic partial
    differential equations(??????????-???????) that
    contain many thousands of terms. Despite more
    than 80 years of intense analytical study, these
    equations have yielded only a handful of special
    solutions relevant for astrophysics and
    cosmology, giving only tantalizing snapshots of
    the dynamics that occur in our universe.

26
  • Scientists have gradually realized that
    numerical studies of Einsteins equations will
    play an essential role in uncovering the full
    picture. Realizing that this work requires new
    tools, developers have created computer programs
    to investigate gravity, giving birth to the field
    of numerical relativity. Progress here has been
    initially slow, due to the complexity of the
    equations, the lack of computer resources, and
    the wide variety of numerical algorithms,
    computational techniques, and underlying physics
    needed to solve these equations.

27
  • A realistic 3D simulation based on the full
    Einstein equations is an enormous task A single
    simulation of coalescing neutron stars or black
    holes would require more than a teraflop per
    second for reasonable performance, and a terabyte
    of memory. Even if the computers needed to
    perform such work existed, we must still increase
    our understanding of the underlying physics,
    mathematics, numerical algorithms, high-speed
    networking, and computational science. These
    cross-disciplinary requirements ensure that no
    single group of researchers has the expertise to
    solve the full problem.

28
  • Further, many traditional relativists trained
    in more mathematical aspects of the problem lack
    expertise in computational science, as do many
    astrophysicists trained in the techniques of
    numerical relativity. We need an effective
    community framework for bringing together experts
    from disparate disciplines and geographically
    distributed locations that will enable
    mathematical relativists, astrophysicists, and
    computer scientists to work together on this
    immensely difficult problem.

29
Some examples
  • Figure 1. Gravitational waves from a full 3D
    grazing merger of two black holes. The image
    shows the objects immediately after the
    coalescence, when the two holes (seen just
    inside) have merged to form a single, larger hole
    at the center. The distortions of the horizon
    (the Gaussian curvature of the surface,????)
    appear as a color map, while the resulting burst
    of gravitational waves (the even-parity
    polarization or real part of Y4) appears in red
    and yellow.

30
  • Figure 2. Additional polarization of
    gravitational waves (imaginary part of Y4) from a
    3D merging collision of two black holes. The
    merged single black-hole horizon can just be seen
    through the cloud of radiation emitted in the
    process.

31
  • Figure 3. Close-up of the horizonwith
    Gaussian curvature to show the distorted nature
    of the surfaceof a black hole formed by the
    collision of two black holes. The two individual
    horizon surfaces can just be seen inside the
    larger horizon formed during the collision
    process.

32
  • Figure 4. Gravitational waves and horizon of
    a newly formed black hole, caused by massive
    collapse of a strong gravitational wave on
    itself. The dotted surface shows the horizon,
    where green colors indicate high curvature and
    yellow means zero curvature. The highest
    curvature indicates the largest gravitational
    radiation. The distortion (the non-sphericity)
    of the black hole radiates away over time, in
    accordance with mathematical theorems about black
    holes.

33
  • Figure 5. Horizon of a gravitational wave
    that implodes to form a black hole, with leftover
    waves escaping, shown at a later time in the same
    evolution presented in Figure 4. We see that the
    horizon curvature is affected by, and correlated
    with, the evolving gravitational wave.

34
Episode ThreeWaveToy Demo
35
including
  • Remote monitoring and steering of an application
    from any web browser
  • Streaming of isosurfaces(???) from a simulation,
    which can then be viewed on a local machine
  • Remote visualization of 2D slices from any grid
    function in a simulation as jpegs in a web
    browser

36
  • The application we are using is the
    simulation of the 3D scalar field produced by two
    orbiting sources. The solution is found by finite
    differencing a hyperbolic partial differential
    equation(????????) for the scalar field. This is
    a very simple application, however it is
    representative of a large class of more complex
    systems, including Einstein's Equations,
    Maxwell's Equations, or the Navier-Stokes
    Equations. We use it for demonstrations since the
    simulation is not computationally intensive, is
    very robust, has simple parameter choices, and
    has reasonable graphics.

37
Before you start, make sure you have the
following items
  • GetCactus the perl script for easily checking a
    Cactus application out from our CVS server.
  • WaveDemo.th the ThornList for the demo, this is
    used to tell GetCactus which thorns to get.
  • WaveDemo.par a parameter file for running the
    demonstration.
  • IsoView the isosurface visualization client.
  • A web browser.
  • Note that you'll need a live network connection
    to checkout the code, but you can run the demo on
    a single machine, the remote tools will look more
    impressive though if you use two networked
    machines, preferably a long way apart.

38
Check out and compile
  • Checkout the source code using something like
  • perl GetCactus WaveDemo.th
  • You should be able to use the default answers for
    all the questions
  • Move into the Cactus directory (cd Cactus), and
    compile the application using either
  • gmake WaveDemo-config ltconfiguration optionsgt
  • gmake WaveDemo

39
  • or if you have a configuration file (this is
    easiest, you don't need to remember the options
    you use)
  • gmake WaveDemo-config optionsltconfiguration
    filenamegt
  • gmake WaveDemo
  • Hopefully that went OK, and you now have an
    executable, exe/cactus_WaveDemo. Check it really
    worked by running the testsuites, just type
  • gmake WaveDemo-testsuite
  • and use the default answers to each question.

40
Run the demo
  • Move the downloaded demo parameter file into the
    Cactus directory. To start the simulation, run
    your new executable with the demo parameter file,
    if you have a single processor executable
  • ./exe/cactus_WaveDemo WaveDemo.par
  • If you compiled with MPI and have a
    multiprocessor version, you will need to use the
    appropriate mpi command for running.

41
  • When the simulation starts, you will see output
    describing for example the activated thorns and
    the scheduling tree.
  • If you have the simple visualization client
    xgraph installed, you can look at the 1D output

42
Connecting with a web browser
  • To connect to the simulation, move to another
    machine if you have one, and start up a web
    browser. Connect to
  • http//ltmachine namegt5555
  • where ltmachine namegt5555 is the name of the
    machine where the simulation is running. Note
    that this information was part of the standard
    output when the simulation started for example
  • Server started on http//gullveig.aei-potsdam.mpg.
    de5555/
  • Now you should see a screen with information
    about the simulation.

43
(No Transcript)
44
Viewing IsoSurfaces
  • Start up the IsoView client, using
  • IsoView -h ltmachine namegt -dp 5557 -cp 5558
  • Again, this information can be found in the
    standard output, for example
  • Isosurfacer listening for control connections on
    gullveig.aei-potsdam.mpg.de port 5558/
  • Isosurfacer listening for data connections on
    gullveig.aei-potsdam.mpg.de port 5557/

45
You should now see rotating blobs appearing in
the client, looking something like this
46
Steering the Simulation
47
If you are watching the isosurfaces you should
see the blobs move together.
48
Episode FourSome Other Sites
  • NCSA Datalink Article about Cactus from the NCSA
    Datalink news letter. http//archive.ncsa.uiuc.edu
    /datalink/9911/Cactus1.html
  • TASC Review Review of Cactus Framework by
    NASA/TASC http//sdcd.gsfc.nasa.gov/ESS/esmf_tasc/
    Files/Cactus_b.html
  • IEEE Computing Cover story article about Cactus
    in IEEE Computing. http//www.computer.org/compute
    r/articles/einstein_1299_1.htm
  • Albert Einstein Institut The birth place of the
    Cactus Code. http//www.aei-potsdam.mpg.de/

49
  • Thank you!
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