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3D Numerical Simulation of a Geomagnetic Field Reversal
Los Alamos National Laboratory / Pittsburgh Supercomputing Center
Los Alamos, NM
USA
Year: 1996
Status: Finalist
Category: Science
Nominating Company: Cray Research, Inc.
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Three-dimensional supercomputer simulation of the earth's magnetic
field, using 5,000 hours of computer time to simulate 80,000 years of
history provides new insights into the way the earth works. |
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Man has been aware of the Earth's magnetic field for thousands of
years and has used it for navigation for hundreds of years. The field
has protected life on Earth by providing a magnetic shield against
solar cosmic rays. Palaeomagnetic records show that it has existed
for more than a billion years; and it probably has existed since the
Earth's beginning. Yet, based on the Earth's dimensions and
electrical conductivity, the free decay time for the Earth's field is only
about 13,000 years; so scientists have long postulated that there
must be some mechanism that continually regenerates the field.
Understanding the Earth's magnetic field requires a model that
reproduces its salient features: a field that is maintained for many
magnetic decay times, is dominantly dipolar at the surface with a
dipole axis that on the average lies close to the geographic axis of
rotation, exhibits secular variation of the non-dipolar structure on
time scales of ten to a hundred years, and has occasional reversals
of the dipole polarity that take a few thousand years to complete and
occur a few hundred thousand years apart. According to Merrill &
McElhinny (in "The Earth's Magnetic Field", Academic Press, 1983),
Albert Einstein considered understanding the origin of the Earth's
magnetic field as being one of the five most important unsolved
problems in physics.
Gary A. Glatzmaier (Los Alamos) and
Paul H. Roberts (UCLA) have recently developed the first fully
self-consistent three-dimensional (3D) numerical model of the
"geodynamo", the mechanism in the Earth's core that generates and
maintains the geomagnetic field. With this model, running on
computers at the Pittsburgh Supercomputing Center, they
have produced a successful simulation of the Earth's field that is
providing answers to many fundamental questions about the field's
structure and evolution.
The computer model solves the
nonlinear magnetohydrodynamic (MHD) equations that govern the
3D structure and evolution of an electrically-conducting fluid
undergoing convection in a rapidly-rotating spherical shell, their
model of the Earth's outer liquid core. Convection is driven by both
thermal and compositional buoyancy sources which develop at the
boundary between the solid inner core and the outer liquid core (the
inner-core boundary, ICB). As the core slowly cools, iron in the liquid
iron alloy freezes onto the solid inner core, precipitating the lighter
constituent (e.g., silicon), which is compositionally buoyant. Latent
heat is also given off in this process, providing a source of thermal
buoyancy. In the model, the local fluxes of light constituent and latent
heat at the ICB are both proportional to the local, time-dependent
cooling rate at the ICB. Heat is transferred out of the core at the
boundary between the outer liquid core and the solid mantle above
(the core-mantle boundary, CMB) according to the Earth-like heat flux
pattern they specify at the CMB. The resulting convection in the outer
liquid core, influenced by the Earth's rotation, twists and shears
magnetic field, generating new magnetic field to replace that which
diffuses away. The generated magnetic field diffuses into the solid,
electrically-conducting, inner core providing magnetic torque
between the inner and outer cores. Magnetic torque also exists
between the outer liquid core and a solid mantle above via a thin
conducting layer just above the CMB. The rest of the mantle is
assumed an insulator since its conductivity is so small compared to
the conductivity of the core; so the external magnetic field above this
layer at the CMB is a source-free potential field. Time-dependent
rotation rates of the solid inner core and solid mantle are determined
by the net torques at the ICB and CMB, respectively.
The model
prescriptions (mass, dimensions, rotation rate, material properties,
specified heat flux at the CMB) are, as much as possible, Earth-like.
The resulting simulated magnetic field has so far been maintained
for more than 80,000 years (six magnetic decay times), with no
indication that it will decay away. The strength and
dipole-dominated structure of the magnetic field at the surface of the
modeled Earth is very similar to that measured on the Earth; and the
secular variation of the non-dipolar structures of the field is
characterized by a westward drift, similar to that seen in the Earth's
field. However, besides demonstrating for the first time that the
Earth's magnetic field could be generated by a convective dynamo
mechanism, the really exciting feature of the simulation is a reversal
of the dipole polarity that occurs about 36,000 years into the
simulation and takes a little more than a thousand years to
complete, after which the field does not reverse again during the
remaining 44,000 years of the simulation. This first 3D simulation of
a magnetic field reversal has several properties (like a significant
decrease in the magnetic field strength during the reversal and
recovery after the reversal) similar to those seen in the Earth's
palaeomagnetic reversal record captured in rocks and
sediments.
Slides 1-3 show snapshots of the structure of the
simulated 3D magnetic field, which is portrayed via lines of force that
are drawn out to two Earth radii and colored gold where the radial
component of the field is directed outward and blue where it is
inward. The striking transition from the relatively smooth structure of
the potential field outside the core to the much more complicated
and intense field structure inside the core occurs at the CMB. The
field outside the core usually has a dominantly dipolar structure as
seen before (Slide 1) and after (Slide 3) the reversal with the dipole
axis nearly aligned with the rotation axis, which is vertical in these
figures. This simulation provides, for the first time, answers to the
long-standing questions of why the Earth's magnetic field is so
strongly dipolar and why the dipole axis is closely aligned with the
rotation axis of the Earth. To understand this, consider the snapshot
of one component of the simulated fluid flow that is illustrated in
Slide 4 in which regions of strong eastward flow are colored gold
and regions of strong westward flow are blue. There is an imaginary
cylinder within the liquid core (tangent to the inner core and parallel
to the rotation axis, see Slide 4) on which large shears in
the east-west flow develop due to the effects of rotation, the
spherical geometry, and the solid inner core. These shears generate
strong magnetic field by stretching it out in an east-west orientation
(see Slide 3). The tangent cylinder intersects the CMB in the polar
regions and so provides a large supply of outward directed field at
one pole and inward directed field at the other pole to maintain the
external dipolar structure that has its axis nearly aligned with the
rotation axis.
The reversal of the dipole polarity is illustrated in
Slides 1-3. Notice how, at the top of the figure, the field is directed
outward before the reversal (Slide 1) and inward after the reversal
(Slide 3). During the middle of the polarity transition (Slide 2) the field
structure at the surface is much more complicated and its dipolar
part, which no longer dominates at this time, has an axis that
passes through the equatorial plane. A movie of this simulation
shows how the field in the outer liquid core is continually attempting
to reverse its axial dipole polarity on a short time scale (roughly 100
years) corresponding to convective overturning but usually fails
because the field in the solid inner core, which can only change on a
longer diffusive time scale (about 2000 years), usually does not have
enough time to completely diffuse away before it is re-generated at
the ICB. Once in many attempts the 3D configurations of the
buoyancy, flow, and magnetic field in the outer core are right for a
long enough period of time for the inner core axial dipole field to
diffuse away, thus allowing the reversed axial dipole field in the outer
core to diffuse into the inner core and establish the new reversed
polarity. This simulation suggests that the strong nonlinear feedback
in three dimensions and the different time scales of the liquid and
solid cores are responsible for the Earth's stochastic reversal
record. |
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The Glatzmaier-Roberts simulation of the geodynamo has provided
answers to several long-standing questions (as discussed in the
previous section) about the Earth's magnetic field that have arisen
from both palaeomagnetic and more contemporary geomagnetic
measurements. As a result of this one simulation, palaeomagnetic
and geomagnetic observational researchers have this year, for the
first time, actively sought to collaborate with the geodynamo
modeling community. Previous models of the geodynamo were
always too unrealistic and non-unique because the full set of
equations was never self-consistently solved; they typically were only
two-dimensional and employed ad hoc, prescribed flows instead of
solving for 3D fluid flow with the magnetic field. As a result these
previous models never demonstrated that the Earth's field could be
generated by a convective dynamo and never produced a field like
the Earth's field. The collaboration that has begun will
provide feedback between those who have been measuring the
Earth's field and those who have been modeling it, which will benefit
both communities. Already the simulation has provided support for
the traditional palaeomagnetic assumption that the Earth's field is
usually dipole dominated. However, the simulation has also
provided reason to suspect that the assumption the Earth's field is
dipole dominated during its reversals, which palaeomagnetic
reversal studies have long relied on, may not be a valid one.
Palaeomagnetic reversal studies are now beginning to account for
the quadrupole part of the field in addition to the dipole
part.
This year the Glatzmaier-Roberts geodynamo simulation
has created new excitement not only for scientists who measure and
model the Earth's field, but for many scientists outside geophysics
and laymen who have a strong curiosity about the Earth's magnetic
field and wish to improve their understanding of the environment they
live in. This has become evident by the publicity these results have
received this year in the press (as discussed in the next
section).
The simulation has also provided a basis for
understanding, and maybe someday predicting, the secular variation
in the Earth's field as seen at the surface. Small changes in the local
direction of the field occur continually; this is one reason why
regional charts and maps (Slide 5) that show magnetic North relative
to geographic North are typically updated every ten
years.
The axial dipolar structure of the Earth's magnetic field,
through its interaction with the solar wind, creates a magnetosphere
around the Earth that shields life from harmful solar cosmic
radiation. However, the simulation indicates that during a magnetic
reversal the field strength above the surface is much weaker; so the
magnetosphere would be smaller, which could affect the structure
and size of the Earth's ionosphere, stratosphere, and protective
ozone layer. In addition, the equatorial directed magnetic dipole
during a reversal (Slide 2) rotates with the diurnal rotation of the
Earth, probably resulting in a very different type of magnetosphere
that may not provide an effective shield against cosmic radiation.
This modified magnetic and radiation environment during a
magnetic reversal, besides no longer providing a reliable means of
navigation for birds, could affect the survival and evolution of many
species.
Much research needs to be done to improve our
understanding of magnetic reversals and their environmental
consequences. Fortunately, there is plenty of time to conduct these
studies before the next one occurs since magnetic reversals take a
few thousand years from start to end. However, the last magnetic
reversal occurred about 780,000 years ago; so we may be overdue.
The Earth's magnetic field strength has been decreasing since
scientists began monitoring it 150 years ago, which according to the
reversal simulation could be an indication that a magnetic
reversal may be about to begin. On the other hand, the present
decline in the field strength may just be a fluctuation. More
collaborative research by observational and computational scientists
should uncover more definitive precursors of a reversal. |
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Information technology has played an important role in this project
at several levels, from the methods for computing the numerical
solution to the methods of communicating the results to others. The
numerical model grew out of models that had originally been
developed by Glatzmaier over a decade ago to simulate convection
and magnetic field generation in the sun's interior. However, as
discussed in the last section, the physical conditions in the liquid
core of the Earth (e.g., the large Coriolis and magnetic Lorentz forces
compared to the small viscous and inertial forces) required the
development of a new, more sophisticated numerical method that is
more accurate and stable. The code, which is highly vectorized, is
also parallelized for parallel processing on
today's supercomputers.
Glatzmaier developed, tested,
and debugged the computer code at the Los Alamos National
Laboratory, but did the production runs on the Cray C-90 computer at
the NSF Pittsburgh Supercomputing Center, which at the time was
the best computer for this problem. Roberts, at UCLA,
provided strong theoretical guidance in the development of the
model and in the analysis and physical interpretation of the solution.
The 80,000-year simulation required more than 5000 hours of cpu
time and took over two years to accomplish. The simulation was
broken into many individual runs, each typically spanning 500 years.
The jobs were submitted remotely from Los Alamos over the Internet
and the progress was checked daily. Data files produced by each job
were routinely transmitted over the Internet back to Los Alamos for
analysis. This daily reliance on the Internet to remotely run a large
problem over a period of two years demonstrated that computational
scientists no longer need to work where the supercomputers are
located. It also allows scientists to easily run their computer codes
on new computers that become available in other places. Soon the
Glatzmaier-Roberts code may be running on massively parallel
computers at Los Alamos and at various other centers around
the Country.
Analyzing the 3D, time-dependent,
multi-variable solution required new visualization tools. For example,
Glatzmaier developed the program that generates the 3D graphical
data from a snapshot of his solution that he then inputs to the
commercial software, AVS (Advanced Visual Systems), that
produces the images of the 3D vector field in terms of lines of force
(Slides 1-3). He also developed programs that he used to
make several graphical movies of the simulated magnetic reversal.
These images and movies proved to be extremely valuable for
analyzing and understanding the 3D structure and evolution of the
field. They were also valuable for describing the solution and
explaining the dynamo mechanism to others both in written
publications and oral presentations.
The results were initially
communicated in two refereed papers by Glatzmaier and Roberts ("A
three-dimensional convective dynamo solution with rotating and
finitely conducting inner core and mantle" Physics of the Earth and
Planetary Interiors, vol. 91, 63-75, 1995; and "A three dimensional
self-consistent computer simulation of a geomagnetic field reversal"
Nature, vol. 377, 203-209, 1995). The second article was featured on
the cover of Nature on September 21, 1995. Since then there has
been an explosion of publicity regarding this simulated
geomagnetic field reversal. Several newspapers in at least five
countries covered the story (e.g., the Washington Post, on
September 25, 1995). Several scientific magazines also wrote
follow-up articles. Articles appeared in EOS (American Geophysical
Union), the American Institute of Physics Bulletin, Geotimes
(American Geological Institute), PSC News, Scientific Computing
World magazine (England), GEO magazine (Germany),
FACTS magazine (Switzerland), and in the January 1996 issue of
Physics Today which also featured it on the cover. Articles are also
about to appear in Eureka magazine (France) and Science et Vie
magazine (France). For several of these articles, color figures
(similar the those in Slides 1-4) were sent over the Internet to the
magazines for their use. The popularity of these results has
apparently been due to the familiarity most people have with the
concept of the Earth's field and the easy way of relating a magnetic
field reversal to a compass needle pointing south instead of north
(Slide 5). Even though the details of the physics and the
computations are complicated, the basic concepts are
familiar.
So far Glatzmaier and Roberts have given about 15
invited talks on their results at universities and other scientific
institutions in the USA and 5 invited talks in Europe. In these talks,
the computer graphical slides and movies of their simulated
magnetic field reversal were always very helpful for describing the
3D structure and time dependence of the field. Copies of their video
movies were also given, upon request, to universities in the USA, the
UK, Australia, Bulgaria, and Japan; and they are now part of the
"Time Capsule" for the Smithsonian collection. |
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This is the first 3D self-consistent numerical simulation of
the geodynamo and of a geomagnetic field reversal. The only other
effort to develop a geodynamo model in the USA is at Harvard
University. Efforts are also underway in the UK, Australia, Japan,
Germany, and France.
The Glatzmaier-Roberts geodynamo
model was the 40th version of a model that originally was developed
by Glatzmaier to simulate the solar dynamo (Glatzmaier "Numerical
simulations of stellar convective dynamos. I. The model and method"
Journal of Computational Physics, vol. 55, 461-484, 1984). Each
version tested a different numerical method, attempting to overcome
numerical difficulties (described ahead). Finally, after several years
of development and testing, the 40th version proved robust enough
to accurately and efficiently solve the full set of nonlinear equations
and produce the first geodynamo simulation. |
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The original goal of this project was to test if a convective
dynamo within the parameter regime appropriate for the Earth could
generate and maintain a magnetic field without decaying away. This
has been postulated for about 40 years but, until now, never
demonstrated. The Glatzmaier-Roberts geodynamo simulation has
now clearly demonstrated that it is possible and has shown how the
geodynamo mechanism works. In addition, it has provided answers
to long-standing questions like why the Earth's field is dominantly
dipolar with a magnetic axis nearly aligned with the Earth's rotation
axis and how the secular variation of the non-dipolar part of the field
occurs. Finally, the simulation unexpectedly demonstrated how a
magnetic field reversal can occur and why the times between
reversals are long and differ so greatly.
Future plans for this
project call for improved representations of the physics. In particular,
more studies will be done to better understand what forces at the
CMB may trigger a field reversal. For example, the effects of torques
between the liquid core and the solid mantle resulting from
topography at the CMB will be investigated; and the effects the
precession of the mantle due to the gravitational forces of the sun
and moon may prove to be important to the dynamics of the
liquid core. In addition, there are plans to use the simulated
3D time-dependent magnetic field as input for a different model
that computes the magnetosphere resulting from the interaction of
the Earth's field and the solar wind in order to study the structure and
evolution of the magnetosphere during a magnetic reversal. |
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The magnetohydrodynamic equations describe how the fluid
temperature, density, pressure, gravitational potential, light
constituent concentration, flow velocity, and magnetic field all vary in
three dimensions and time and how they all provide nonlinear
feedback on the others. Every time the computer solves this large set
of coupled equations the solution is advanced 30 days everywhere in
the Earth's core and, for the external magnetic field, well beyond the
core. The numerical difficulty is that the viscous forces in the
modeled core are typically five orders of magnitude smaller than the
Coriolis forces (due to rotation) and the Lorentz forces (due to
electric currents flowing across magnetic field). Consequently, to
have a stable and accurate code for the parameter regime
appropriate for the Earth, the Lorentz forces were treated explicitly
(i.e., using present and past information to advance the solution)
while the Coriolis forces were treated implicitly (i.e., using future
information). The resulting coupling between spherical harmonic
coefficients of the solution required a new method (version 40) that
involved the construction of large block-banded matrix equations that
are solved each 30-day timestep.
After several years of
development, this robust code then required over 5000 cpu hours of
supercomputer time to simulate the 80,000 years. This was
accomplished remotely over the Internet between Los Alamos and
the Pittsburgh Supercomputing Center. This large computing
resource was obtained by writing proposals that successfully
competed nationwide for NSF computing resources over a period of
two years.
Besides the technical difficulties involved in the
development and computation of this numerical study, there were
psychological difficulties. Glatzmaier and Roberts set out to develop
a computer model that would solve a complex problem that many
other very capable scientists failed to solve. The many years of hard
work and frustration when methods would not work required
perseverance, especially when there seemed to be so little chance
for success. However, the challenge and hope for success was
addicting; and the investment eventually paid off beautifully. The
excitement felt by Glatzmaier and Roberts is now shared by many. |
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