October 6-10, 1997
Introduction, (Mark Tillack, UCSD)
During the past 33 years, the Institute of Electrical and Electronics Engineers (IEEE) Nuclear and Plasma Systems Society (NPSS) Symposium on Fusion Engineering (SOFE) has been a leading technical forum for exchange of information on the engineering and technology of fusion energy. The 17th Symposium was held October 6-9, 1997 in San Diego, California. This report includes a brief summary of each technical session written by the session chairpersons. The Symposium proceedings, including full papers for each presentation, will be published by the IEEE.
Eleven plenary speakers provided the backbone of the symposium:
M. Keilhacker: Deuterium-Tritium Experiments in JET and Their Implications
for ITER
M. Cambell: Recent Accomplishments in ICF
D. M. Meade TFTR Retrospective
A. Sakasai: High Performance and Steady-State Experiments on JT-60U
P. I. Petersen: Results from the DIII-D Tokamak
J. H. Irby: The Alcator C-Mod Tokamak and Recent Results
O. Motojima: Review of Engineering Progress in LHD Project
V. Erckmann: The W7-X Project: Scientific Basis and Technical
Realization
R. Aymar: Status and Prospects of ITER
J. Paisner: The National Ignition Facility for Inertial Confinement
Fusion
R. W. Conn: From ITER and NIF to an Attractive Commercial Energy
Source
Twelve oral sessions included both invited and contributed lectures:
O1: Tokamak Engineering and Operations
O2: Safety & Environment and Power Plants
O3: New Machines
O4: Tritium Systems and Tritium Control
O5: Plasma-Facing Component Technology
O6: Heating and Current Drive Systems
O7: Plasma Control and Power Systems
O8: Inertial Fusion Engineering: Targets, Drivers & Chambers
O9: Magnet Systems
O10: Physics and Advanced Devices
O11: Next Generation ICF Devices
O12: Data Acquisition and Diagnostics
The majority of the presentations were provided in 23 poster sessions:
P1: Magnet Systems - I
P2: Safety & Environment - I
P4: Divertor and Plasma-Facing Component Engineering - I
P5: Data Acquisition and Diagnostics
P6: Magnet Systems - II
P7: Nuclear Engineering
P8: Materials Engineering
P9: Tritium Systems
P10: Vacuum Systems
P11: Plasma-Material Interactions and In-Vessel Tritium Control
P12: Safety & Environment - II
P13: Divertor and Plasma-Facing Component Engineering - II
P14: Electromagnetics and Electromechanics
P15: Assembly, Fabrication and Maintenance
P16: Plasma Control and Control Systems
P17: New and Proposed Machines
P18: Inertial Fusion Engineering
P19: Plasma Physics
P20: Blanket, Shield and Vacuum Vessel Engineering
P21: Power Plant Studies
P22: Neutral Beam Injection and Fuelling Systems
P23: Power Systems
The Technical Program Chairman for the Symposium was Mark Tillack (UCSD), who was supported by co-chairmen Ken Schultz (GA), Phil Heitzenroeder (PPPL), and Wayne Meier (LLNL). Session chairmen are identified below, together with the sessions they chaired.
Plenary Session L1, Ken Schultz (GA) and Valerie Chuyanov
(ITER-US)
The opening plenary session of the Symposium established the ecumenical tone
that was evident throughout the meeting by having presentations on recent
exciting events in both the magnetic side and the inertial side of the world
fusion program.
At the first lecture Dr. Martin Keilhacker, Director of the JET Joint
Undertaking, presented the latest results of JET's D-T experiments and their
implications for ITER. In D-T experiments performed during the last several
weeks before the Symposium, JET established a new record for fusion power
production with 13 MW of fusion power and up to 14 MJ of fusion energy per
pulse. It produced a total of 340 MJ of fusion eneergy in 100 full D-T pulses
and achieved energy amplification of Q = 0.6. This series of experiments
enabled the JET staff to study the scaling of important physical phenomena with
ion mass. The results were overall quite favorable for ITER.
It was found that the power threshold of the H-mode has a strong favorable
dependence on ion mass, ~ 1/A. It the same time, the energy confinement is
practically independent of ion mass. While it would be beneficial for ITER if
there were a positive dependence of confinement on mass, this effect is more
than compensated by a stronger than expected dependence of confinement on
density. Energy confinement scaling was found to be close to Gyro-Bohm, but
without mass dependence. Studies of the JET plasma edge parameters have shown
that the edge gradients scale as T1/4. This is consistent with
confinement scaling as (a.r)1/2,
which is also favorable for
ITER. About half of the heating power was provided by fusion alphas and the
effects of this heating were observed. No negative effects connected with
Alfvén eigenmodes driven by alpha particles have been observed.
These positive results bode well for the fusion program and for the recent
proposal to extend JET operation through 2003 with extensive studies of open
and closed divertor geometry followed by another program of D-T experiments.
The second presentation was given by Dr. Michael Cambell, Associate Director of
Lawrence Livermore National Laboratory (LLNL) for Laser Programs, summarizing
recent accomplishments in the Inertial Confinement Fusion (ICF) Program. He
began with an overview of the National Ignition Facility (NIF) project that
just broke ground at LLNL. This 1.8 MJ, 500 TW laser is the culmination of 25
years of R&D on ICF at LLNL, Los Alamos National Laboratory (LANL) and the
University of Rochester Laboratory for Laser Energetics. It is designed to
achieve ignition and modest energy gain. Both indirect drive and direct drive
implosion experiments will be possible in this facility which will be an
important element in DOE's "science based stockpile stewardship" program, and
also will allow significant advances in R&D on inertial fusion energy
applications.
The science and technology needed for the NIF have been developed on
experiments such as the Beamlet at LLNL which is a full scale prototype of one
of the 192 NIF beamlines, and through an extensive program of industrial
facilitization to develop the capacity to produce the quantities of large, very
high quality laser components the NIF will need. The scientific basis for
ignition has been developed over the years through extensive programs of
experimentation and analysis of the physics of laser-plasma coupling, implosion
symmetry control and hydrodynamic stability on the Nova and Omega lasers and
other ICF program facilities. Important developments have included recognition
of the need for and the techniques to achieve laser beam smoothing by
mechanisms of introducing incoherence.
The target designs for ignition include both direct and indirect drive
candidates with both beryllium and plastic capsules, so there are multiple
options for ignition, giving a robust program. The heart of all target designs
will be a spherical shell of frozen D-T, made by techniques being developed by
LLNL, LANL and General Atomics. The NIF will develop the physics basis for
inertial fusion energy (IFE) applications, and will permit some IFE technology
development, but NIF will only shoot a few targets each day and IFE must shoot
a few every second.
To develop a rep-rated laser for IFE application LLNL is now constructing the
Mercury laser, a 0.1 kW, 10 Hz diode-pumped solid state laser (DPSSL) that
should achieve efficiency of 10% or more. The DPSSL also will allow
application of the "chirped pulse amplification" technique, wherein laser
pulses are stretched, amplified and recompressed to obtain petawatt power laser
pulses. These intense pulses offer the possibility of igniting a cold
compressed target at much lower energy than "conventional" ICF, raising the
possibility for very high gain and a low cost path for IFE development.
Further, these intense pulses offer exciting potential for materials processing
and biomedical application.
Plenary Session L2, Michael Williams (PPPL) and Phillip Heitzenroeder
(PPPL)
Dr. Dale Meade of the Princeton Plasma Physics Laboratory presented the opening
talk of this session: "TFTR - A Twenty Year Retrospective". He began with a
reminder of the general political environment twenty years ago when TFTR was
being constructed. Memories of gas rationing and heating oil shortages were
still strong, energy was a major public issue and fusion budgets were strong.
This contrasts with the present situation, where fuel supplies appear to be
plentiful, the budget deficit is a major issue and fusion budgets have been
declining. The major fusion issues twenty years ago were confinement scaling,
MHD stability, impurity control, fusion power production and large scale
engineering and operation of D-T devices. During those twenty years, the
widely used Lawson criteria
niTitE used as
a measure of fusion progress has increased by a factor of 1000 -- from 0.01 x
1020 to 10 x 1020 m-3 s keV.
TFTR demonstrated the maturity of fusion engineering and helped provide
confidence that a large-scale tokamak can be designed to meet specifications,
achieve cost and schedule goals and be operated safely and reliably. TFTR
operated with D-T for more than 3 years, producing over 1090 D-T discharges and
1.5 GJ of fusion energy. TFTR's highest power plasmas produced 10.7 MW of
fusion power with fusion power densities in the core exceeding those expected
for ignited plasmas producing 1500 MW in ITER. In spite of operating in a D-T
environment with its attendant activation and strict safety requirements, TFTR
had >85% availability and the neutral beams were operated above their
original design ratings (40 MW vs. 33 MW), as were the TF coils (6 T
vs. 5.2 T). Early D-T experiments demonstrated a favorable "isotopic"
scaling with D-T plasmas and confirmed the ITER ICRF heating mode using second
harmonic tritium resonance. TFTR's "ITER-like" plasma core conditions, coupled
with comprehensive D-T diagnostics, allowed detailed measurements of alpha
particle energy distributions which were used to test calculations of alpha
particle dynamics. TFTR made the first direct observations of alpha heating
and alpha driven instabilities in a tokamak. It also performed detailed
studies of plasma turbulence and transport, sheared plasma flow, and sheared
magnetic fields that demonstrated the limitations of the traditional empirical
scaling models and led to the development of new models of plasma transport
based on marginal stability and sheared plasma flow. In looking towards the
future, Dr. Meade feels that these experiments and theoretical models indicate
the possibility of increasing the fusion power production in TFTR to over 20 MW
with new opportunities for studies of strong alpha heating with only a modest
extension of TFTR operating regimes.
Dr. A Sakasai of the Japan Atomic Energy Research Institute followed with his
talk entitled "High Performance and Steady State Experiments on JT-60U". The
objectives of JT-60 research are to establish the physics basis for a steady
state tokamak fusion reactor and contribute to ITER physics R&D. JT-60U
has made significant progress in support of these objectives in key areas such
as improved confinement, radiative divertor, and non-inductive current drive.
Improved confinement regimes with reversed shear and high
bp
H-modes were successfully developed in 1996. Triple products as high as 1.5 x
1021 m-3 s keV and a world record temperature of 45 keV
were achieved.
Dr. Sakasai noted that the reversed shear configuration is one of the leading
scenarios for steady state tokamak operation. The JT-60 U reversed shear
experiments produced a QDTeq of 1.05 with a record stored
energy level of 10.9 MJ at a plasma current of 2.8 MA. Negative ion based
neutral beam (NINB) experiments also were performed in 1996 in support of the
goal of developing methods for steady state, non-inductive tokamak operation.
The beamline is designed to operate at 0.5 MeV with a total power of 10 MW. In
the initial experiments, 2.5 MW at 350 keV achieved a NB driven current of 0.28
MA with a current drive efficiency of ~8 x 1018 m-2 A/W.
The beam at this energy achieved a high neutralization efficiency of 60%. TAE
mode excitation was observed during NINB injection.
Halo current measurements indicated Ih/ Ip = 0.05 - 0.25
with a toroidal peaking factor (TPF) ranging from 1.4 - 3.6 and the product
Ih/ Ip x TPF < 0.52. A W-shaped pumped divertor
similar to that proposed for ITER was brought into operation in May 1997. Its
pumping speed is 13 m3/s. Experiments are underway to examine
radiative divertor operation with high recycling. Future plans include
construction of a pellet injector capable of continuous pellet injection at 20
Hz and 1 km/s, full current drive at high plasma currents by high power NINB
injection and high performance radiative divertor experiments.
Plenary Session L3, Enzo Bertolini (JET) and Keith Thomassen
(LLNL)
The main features and recent results of the two major tokamaks still
operational in the USA, were presented in this session.
Peter Petersen gave a talk on behalf of the DIII-D Team. Several new systems,
upgrades and repairs were reviewed. A new divertor was installed at the top of
the vessel to pump high triangularity plasmas, and a new view for the motional
Stark effect diagnostics also was installed. Two gyrotrons, rated 1 MW each,
became operational. Steerable mirrors allow the gyrotron to heat the plasma
from the center to the edge. The plasma control has been upgraded to `isoflux'
control and exploits the new real-time plasma equilibrium capability. The
faulty ohmic heating coil has been repaired and the circuit will be
reconfigured to make use of the additional 2.5 Vs. Remote experimental
operations of the machine were done in collaboration with LLNL.
New physics results show that ExB rotational shear causes a transport barrier
in the plasma for the ions and the electrons. VDE's have been studied, and a
toroidal peaking of 4 is seen. Halo currrent can be 30% of the plasma current.
Argon pellets can lower the force and heatloads on the vessel. Additional ECH
power (from 2 to 10 MW) is planned for controlling the plasma profiles.
Divertor development will include pumping in the private flux area, study of a
more closed divertor, and dumping of a double null advanced tokamak shape.
Jim Irby summarized the salient features of the Alcator C-Mod machine, its
construction and engineering features, and its missions in divertors,
transport, and advanced tokamak physics. Recent results from disruption,
H-mode, and electron cyclotron discharge cleaning also were presented. C-Mod
has been operated at 8 T, near its design goal of 9 T, and at currents to 1.5
MA. It is planned to operate up to 2.5 MA in the future, and the rf power will
increase from 4 MW to 12 MW. It operates over the wide density range of n =
0.2 - 15 x 1020 m-3.
One of the major contributions of the C-Mod machine to the tokamak physics and
engineering program is on disruptions and the effects of eddy and halo
currents, which can be rather dramatic at its highest fields. The structures
are already highly stressed at toroidal field currents of 250 kA, with forces
up to 108 N. Consequently, an extensive set of halo diagnostics
have been installed and they first discovered the asymmetry (peaking factors of
1.5 - 2) and scaling of the halo currents (proportional to the square of the
plasma current and inversely with the toroidal field).
In a study of the H-mode transition they note the importance of the plasma edge
and pedestals, and have implemented several new high spatial resolution
diagnostics there. In addition to the existing tangential XUV and poloidal (38
channel) soft x-ray arrays, they plan to add a tangential interferometer and
modification of the core Thomsen system. Their studies have greatly extended
the empirical scaling law of the L-H mode transition, to values of power per
unit of surface of 0.6 MW/m2 and density-field product to 25 x
1020 T-m-3.
Using a 2.45 GHz ECH source of about 3 kW, the cylindrical resonant surface is
swept from the inside to the outside of the vessel for discharge cleaning of
the walls. This results, after about 10 days of continuous operation, in a
clean vessel. New studies to determine the plasma parameters of this ECH
generated plasma have begun, and it is found that the temperature and density
profiles (Te ~ 6-10 eV, ne ~ 1016
m-3) are rather broad, so that sweeping the resonance (which will be
very difficult in large superconducting machines such as ITER) may not be
necessary.
Finally, the planned upgrades of C-Mod over the next two years were described.
In the divertor region, the inner plate will be modified, a bypass flap added,
and full cryopumping installed in the outer divertor. With a prototype pump
they have already reduced the recycling and core impurity concentration by a
factor of 2. Structurally, the divertor will be made compatible with full 9 T
field and 2.5 MA current. There are many planned rf upgrades as well, with a
new 4-strap, 4 MW ICRF antenna constructed by PPPL for single port operation,
and a 4 MW lower hybrid system at 4.6 GHz. Later, another 4 MW ICRF antenna
will be added for a total of 12 MW of rf power.
With these new capabilities in field, current, power, and diagnostics, the
C-Mod program should be able to significantly extend the parameter ranges of
study in their various program missions.
Plenary Session L4, Tom Simonen (GA) and Fred Puhn (ITER-US)
O. Motojima opened the session with his talk entitled: "Review of
Engineering Progress in LHD Project". The LHD project in Toki, Japan is based
on past experience in Japanese original heliotron research. LHD is
approximately 90% complete at this time, and plasma operation is planned to
start in March 1998. It will be the first superconducting helical type device.
The machine has a major radius of 3.9 m, a minor radius of ~0.6 m, a field of 3
Tesla (in Phase I), and ultimately will be equipped with 40 MW of heating
power. The goals of the program are to perform physics experiments that will
extrapolate to breakeven conditions. The operational program will include
demonstrating advanced toroidal operation, confinement improvement, currentless
operation, and use of many generic fusion technologies.
In this paper, he summarized the engineering progress developed during the LHD
device construction which were required to establish the mission of LHD
experiments. The LHD uses NbTi superconducting coils. The helical coil is a
continuous winding incorporating about 36 km of conductor, cooled by pool
boiling liquid helium. It was fabricated using a specially designed helical
coil winding machine. LHD also uses circular poloidal field coils which are
cooled by forced flow liquid helium. The total cold mass of the LHD is about
900 tonnes.
Holding tight tolerances during construction was a critical requirement, and
this has been accomplished successfully using precise and rigid tooling. The
helical coil has a tolerance of +/-2.1 mm on the minor radius and -1.5 mm on
the major radius of the winding. The PF coils have a tolerance of +/-1.4 mm on
the radius and +/-1.5 mm on the height. The welded vacuum vessel had a more
relaxed tolerance of 10 mm.
The first cooldown is planned in January 1998. The cooldown scenario is
carefully programmed to keep the temperature differences in the system below
50K. This results in an initial cooldown time of about one month. The LHD is
expected to produce an equivalent Q of about 0.1 and a temperature of about 10
kev. The program is designed to lead up to a Demo reactor in about 2025.
The second talk, entitled "The W7-X Project: Scientific Basis and Technical
Realization," was presented by V. Erckmann. The W7-X stellarator is in an
early stage of construction in Greifswald Germany. The design is based on
experience with previous stellarators operated in Germany. The goals of the
program are steady-state operation, good confinement, a reactor relevant beta
of ~5%, and development of a divertor. W7-X will have a major radius of 5.5 m,
a minor radius of 0.55 m, and 5 magnetic field periods in the coil system.
W7-X is unique in that it uses modular superconducting coils to provide the
magnetic fields. There are 50 twisted coils of 5 different types in the array.
There are also 20 planar coils used for experimental purposes. The NbTi
superconductor is cooled by forced flow liquid helium. The cold mass is about
350 tonnes. The field at the center of the plasma is 3 Tesla. The conducting
cable incorporates an aluminum jacket, which is aged at elevated temperature
after winding to develop its full structural strength. A prototype coil is now
being built, and will be tested at FZK. In addition, a test section of the
machine is being built, including the cryostat, vacuum vessel, coils, and
ports. This test section will verify the manufacturing tolerances, assembly
procedures, and liquid helium operation.
An important part of the experimental research program is the development of an
efficient divertor configuration. The initial divertor will use a number of
plates which interact with "natural" magnetic islands near the edge of the
plasma. Simulations indicate that the heat deposited on the plates is
accommodated for various operating modes. The divertors are design to handle
10 MW steady state heat load. Cryopumping of the divertor is included in the
design.
Plasma heating will be supplied by ECRH, neutral beam injection, and ICRF. The
ECRH system provides steady state power at 140 GHz. The ECRH system will use
10 units of 1 MW each to provide plasma start-up, profile shaping, and
bootstrap current compensation. The microwave transmission is an optical
system with steerable launchers. The neutral beam will be the type used on
ASDEX-upgrade, and will start out at 5 MW. The machine can be later upgraded
with more neutral beam power and also possibly negative ion beams.
W7-X will be located in a totally new facility at Greifswald. The building
will be completed in 1999, and the machine will be complete in 2004. The
program is intended to show the reactor capability of the stellarator.
Plenary Session L5, Charles Baker (UCSD and ITER/US)
The final plenary session of the conference included three invited papers
covering the two major facilities of fusion R&D, i.e., the
International Thermonuclear Experimental Reactor (ITER) and the National
Ignition Facility (NIF), and a look ahead towards future, attractive fusion
power systems.
The ITER Project Director, Dr. Robert Aymar, presented the status and prospects
of ITER. He reviewed ITER's principal mission, namely to establish the
scientific and technological feasibility of magnetic fusion energy, which is to
be accomplished via an international project involving the European Union,
Japan, Russian Federation and the United States. A comprehensive design has
been developed and will be presented in a Final Design Report in 1998. This
report will include ITER's physics basis, system and component design
descriptions, cost estimates, construction schedules and site requirements.
Dr. Aymar also described the status of R&D activities carried out by the
ITER Home Teams. These activities are focused on seven main projects including
the central solenoid model coil, toroidal field model coil, a section of the
vacuum vessel, first wall/shield modules, divertor cassette and two remote
maintenance demonstrations for the shield modules and divertor cassettes.
Numerous papers were presented at the conference describing many details of the
ITER Project.
Dr. Jeffrey Paisner provided an overview of the NIF Project. The NIF device is
based on a 1.8 MJ, 500 TW laser which is designed to achieve ignited pellet
burns at modest energy gains. The NIF facility is under construction at the
Lawerence Livermore National Laboratory and is scheduled to be completed in
2003. The NIF laser is a neodymium-glass system working at the third harmonic.
The NIF laser and target building will occupy an area of 125 x 170
m2. Key components of the laser system include amplifiers, cavity
filters, a master oscillator, beam transport systems and the final optics
assembly. NIF is designed for both direct and indirect drive pellet
implosions. The total project cost during construction is $1.2B.
Finally, Prof. Robert Conn provided a perspective of the current status and
future outlook of the US fusion program based on recent deliberations of the
Energy R&D Panel of PCAST: the President's Committee of Advisors on
Science and Technology. In 1996, funding needs to continue the US fusion
program with its previous set of objectives became divergent with actual
allocations from Congress. "Restructuring" of the program resulted, with
stronger emphasis on fusion sciences and innovations which could lead to more
attractive end products. The PCAST report attempts to place fusion together
with other energy R&D programs in a context which can provide sustainable
funding. These other programs include end-use efficiency, renewables, fossil
improvements, and advanced fission.
Energy research is being conducted now in a radically changing national and
global marketplace. Deregulation, together with increased concern over the
prospect of global climate change, are affecting energy portfolio R&D
decisions. While on the one hand, the fusion program will continue to support
basic scientific research in high-temperature plasma physics, it also must find
an appropriate strategy to support its energy objectives. For that purpose, we
must address clearly the relationship between developing an attractive fusion
product, the cost of an energy R&D pathway, the changing marketplace, and
the issue of global climate change.
Dr. A. von Halle reported on the final operations of the Tokamak Fusion Test
Reactor (TFTR). In April 1997, TFTR completed its final operating period,
bringing to close a highly successful phase of research in plasma science. The
device produced over 80,000 high power plasmas since 1982 with the objectives
of studying the plasma physics of large tokamaks, gaining experience in the
solution of engineering problems associated with large fusion systems, and
demonstrating fusion energy production from the burning, on a pulsed basis, of
deuterium and tritium in a magnetically confined toroidal plasma system. In
1993, TFTR became the first magnetic fusion device to study plasmas using
nearly equal concentrations of deuterium and tritium. Since that time, over
1000 D-T experimental shots and over 23,000 D-D shots have been carried out
demonstrating new regimes of plasma confinement, proof of alpha heating, and
reactor level fusion power densities by producing a plasma which yielded over
10 MW of fusion power at a corresponding central fusion power density of ~2.8
MWm-3. The TFTR technical systems routinely operated at or beyond
the original design criteria throughout the period, maintaining an impressive
machine availability of >85%. Safe operation in D-T has been demonstrated,
with over 950 kCi of tritium processed within the constraints of a 50 kCi site
limit and a 20 kCi machine limit.
Dr. D. Stork reported on "JET Engineering Development toward D-T Operations in
an ITER-like Machine Configuration". The Joint European Tours (JET) has
recently begun a series of experiments with deuterium-tritium plasmas (DTE1).
These are the first plasma experiments with a 50:50 D-T mixture in a tokamak
with a divertor. Extensive technical work was carried out to ensure that the
JET machine and its major subsystems were able to carry out an extended period
of D-T operation. The JET Active Gas Handing System has supplied around 40 g
of tritium to the Torus and Neutral Beam Injectors (NBI) and has reprocessed
batches of the Torus and NBI. The injection of tritium beams at up to 155 kV
energy and up to total powers of 11.3 MW has taken place. Extensive
deterministic analyses of Design Basis Accidents (DBAs) establish changes
required to protection systems for D-T operation and to satisfy the regulatory
authorities. In the one serious fault which has been encountered in DTE1, the
monitoring systems proved capable of identifying a tiny leak in the TNBI system
(about 7 orders of magnitude below the Design Basis LOCA). Operations were
suspended safely.
Dr. E. Bertolini reported on "Current Engineering Issues and Future Upgrading
of the JET Tokamak". Flexibility and suitable stress margins were included in
the original design, so as to allow modifications and upgrading of the machine
to follow the evolving requirements of the physics issues, i.e.,
toroidal coils, vacuum vessel, additional heating power, and power supply
upgrades.
- The plasma current has been increased up to 7.0 MA, the X-point magnetic
configuration has been established up to 5.0 MA, and the first wall was
progressively covered with CFC or beryllium tiles.
- In this machine configuration, QDTequivalent >1 was
achieved and the first ever controlled thermonuclear experiments in D-T
produced 1.7 MW of fusion power (Nov. 1991).
- The need for active control of the impurities requires an axisymmetric pumped
divertor, which was installed without replacing any of the major components of
the machine.
Further progress in performance can be achieved by increasing the toroidal
magnetic field to 4.0 T. If JET will be extended beyond 1999 and funds will be
made available, additional heating power could be substantially increased and
new machine configurations could be tested. The 15 years of operational
history indicate that JET is an experimental tool that can be rejuvenated, to
make progress in the understanding of fusion physics for several years to come.
Dr. S. Ciattaglia reported on the Frascati Tokamak Upgrade (FTU). About 3500
pulses were performed in the past two years (mostly in D2) with a
toroidal field between 2.5 and 8 Tesla and a plasma current between 0.35-1.3
MA. The main research activities were concentrated on plasma MHD studies with
different heating scenarios. Lower hybrid waves current drive (LHCD) and
electron cyclotron resonance heating (ECRH) were used both alone and together
to investigate synergistic effects. Strong effort was devoted to high density
(1x1020 m-3) current drive experiments and investigating
the possibility of obtaining and sustaining shear reversal configurations.
After a 3-month shutdown planned at the beginning of 1998 to complete
commissioning and debugging of all four ECRH lines, the main program during the
next two years will be largely devoted to experiments with the three rf systems
(LHW, IBM and ECRH). In particular, LHW heating and CD at high density and
high plasma current (1020 m-3/0.5-1 MA) were
demonstrated, combining LHW+ECRH and LHW+IBW injection. Major physics issues
are central heating at high density (~1020 m-3),
transient transport studies, and MHD mode control through ECRH. The long-term
programme envisages studying advanced scenarios (high-beta, large bootstrap
fraction, shaped plasma).
Dr. G. Martin reported on Enhanced Performance for Long Pulses on Tore Supra.
Among the large tokamaks in operation around the world, Tore Supra has the
unique feature of a superconducting magnet which provides a permanent toroidal
field. Its main axis of research is therefore concentrated on the control of
multi-MW plasmas during long duration, with steady-state as an ultimate goal.
Both lower hybrid and fast waves are used to drive the current. Enhanced
performance related to current profile shaping has been intensively studied. A
world record in injected energy was achieved in 1996 with 280 MJ during a two
minute shot. Very long evolution times are then possible in plasma wall
interaction physics.
On the basis of these results, an enhancement in the capability to handle large
power and to control the particles over long duration is planned. This is the
main motivation for the Composants Internes Et Limiteur (CIEL) project, which
consists mainly of upgrading the first wall components:
- A new toroidal belt limiter in the lower of the vessel, which is made from
carbon fibre composite (CFC) brazed on copper tubes.
- A set of pumps to evacuate all types of gas species through the toroidal
throat of this limiter, allowing improved density control.
- A new water-cooled radiation screen to cover as much as possible of the inner
vessel, to avoid uncooled parts interacting with the plasma.
O2: Safety & Environment and Power Plants, L. Topilski
(ITER-US)
"EASY-97: A Multipurpose Activation and Transmutation Code System", by R.
A. Forrest. The European Activation System (EASY) is a complete tool for
the calculation of activation in materials exposed to neutrons up to 20 MeV.
EASY consists of the inventory code FISPACT and the European Activation File
(EAF), which contains various libraries on nuclear data. The EAF-97 library
contains about 12,500 excitation functions involving 766 different targets from
1H to 257Fm, in the energy range 10-5 eV to 20
MeV. Major effort has gone into verification, validation and quality assurance
of EASY-97. This, together with EASY's explicit treatment of uncertainties, is
of great importance as the need to license ITER approaches. For the longer
term, EASY's facilities to analyze pathways of activation product production is
of importance in the optimization of low activation fusion materials.
"Design-Point Determination for the Commercial Spherical Tokamak" by R. L.
Miller. This study was done for the ARIES Team, which provides conceptual
design projections for future commercial fusion power plants, characterizing
their environmental and economic aspects as driven and constrained by presently
understood physics and reasonably extrapolated technology. Interest in the
Spherical Tokamak stems from its high beta and high bootstrap current. As a
result of this study, parameters for a 1-GWe ARIES-ST Commercial-Power-Plant,
including the total capital cost and cost of electricity, were presented for 5
different aspect ratios. Tradeoffs among system power density, recirculating
power, plant availability, technical and operational complexity, and coolant
and structural material choices are resolved in the context of their impacts on
capital and operating costs. The Spherical Tokamak power-plant projection is
somewhat problematic due to issues such as toroidal field coil centerpost,
recirculating power fraction, high power density, etc.
"Identification of Postulated Accident Sequences in ITER", by N. P.
Taylor. For ITER accident analysis to be complete, it must be based on a
comprehensive list of fault conditions, or accident initiating events, covering
all conceivable hazards arising in the plant. Two independent and
complementary approaches have been employed, illustrated in this paper by a
portion of a global fault tree and a sample event tree. These approaches are
the component-level (bottom-up) and the top-down approaches. The former is
based on the application of systematic methods which seek to catalogue all
potential faults in the ITER systems, and to consider the conceivable
consequences of these faults. The focus is on the failure of individual
components, and based on the design in as much detail as available. The
top-down approach starts at the plant level, and takes a global view of the
potential hazards and the safety functions which provide protection. By
considering the abnormal events which could have to occur to realize these
hazards, a list of accident initiators is again produced, in terms of system or
in some cases component faults. Using this approach, the resulting catalogue
of primary initiating events (for ITER accident analysis) and event sequences
have been checked carefully to ensure that each is covered directly and
indirectly, by one of the reference accidents chosen for detail analysis. This
has confirmed that the consequences of all identified accidents are enveloped
by the assessed consequences in one or more of the analyses. Thus, the outcome
of these studies, taken together with the results of reference accident
analyses, gives confidence that the ITER engineering design will achieve its
safety targets.
"Implementation of the ITER Confinement Function", by D. A. Dilling.
This paper summarizes the ITER confinement functional requirements, describes
the confinement strategy for the ITER tokamak, and shows how the design meets
the objectives. All radionuclide sources are confined by at least two
barriers. The first barrier for the ITER plasma and in-vessel deposits is the
vacuum vessel (VV) and the ex-vessel portions of the primary heat transfer
system (PHTS) of the plasma facing components. The second barrier starts with
the cryostat vessel (CV) and is extended to include the heat transfer vaults.
Thus, two critical components are high quality vacuum vessels, which must be
intact for the machine to operate independent of safety considerations.
Features to prevent or limit releases via various penetrations of the VV are
tailored to the characteristics of the potential hazards associated with each
system, as in a chemical plant. This strategy includes first and second
barriers in various heating and current drive systems interfacing with the
plasma. The primary heat transfer coolant is contained by the cooling systems
and by the PHTS vaults that form the second barrier. Outside the second
barrier, some volumes are assigned confinement-related functions and are
equipped with heating, ventilation, and air-conditioning (HVAC) systems which
treat potential releases. These features work together to assure that the
potential impact on public health and safety is within acceptable limits for
all credible challenging events. The paper also includes limited information
on the confinement of sources during maintenance, in the tritium plant, and in
the hot cell building.
"Analysis for the Safety Case for JET D-T Operation", by A. C. Bell.
Approval has been given by appropriate safety and regulatory authorities for
D-T operation of JET with up to 20 g of tritium in torus systems, and for the
generation of 14 MeV neutrons within a limit of 2.5 x 1020. This
permits the DTE1 series of experiments to be performed. The results of the
safety case analysis were presented, concentrating on the methodology of
accident sequence identification. This includes elimination of low
consequences events; the source terms, dose factors and consequences for key
design basis and beyond design basis accidents (such as LOVA, in-vessel LOCA,
ex-vessel LOCA, LOFA, etc.); and the assessed probabilities of such events.
O3: New Machines, Ronald Stambaugh (General Atomics)
The papers in this session covered several initiatives for new fusion devices
around the world.
The KSTAR Tokamak (presented by J. Kim). This paper described the KSTAR
(Korea Superconducting Tokamak Advanced Research) project, the major effort of
the Korean National Fusion Program to design, construct, and operate a
steady-state capable superconducting tokamak. The project is led by Korea
Basic Science Institute and shared by national laboratories, universities, and
industry along with international collaboration. It is in the conceptual
design phase and aims for first plasma by mid 2002. The major design
parameters of KSTAR are major radius 1.8 m, minor radius 0.5 m, toroidal field
3.5 T, plasma current 2 MA, elongation 2.0, triangularity 0.8, and double null
poloidal divertor. The toroidal and poloidal coil magnets are superconducting.
The device is initially configured for a 20 second pulse and then to be
upgraded to 300 second operation with non-inductive current drive. The
auxiliary heating and current drive system consists of neutral beams, ICRF,
lower hybrid, and ECRF. Deuterium operation is planned with full radiation
shielding.
Engineering Overview of the National Spherical Torus Experiment (NSTX)
(presented by C. Neumeyer). This paper described the NSTX Project, a
U. S. national facility for the study of plasma stability, confinement,
heating, and current drive in a low aspect ratio, spherical torus. The major
design parameters of NSTX are major radius 0.85 m, aspect ratio 1.26, toroidal
field 0.3 (0.6) T, and plasma current 1.0 MA. Copper magnets are used
throughout with pulse lengths to be in the range 0.5-5.0 seconds. The
principal design challenge has been the highly compact center stack with a 36
turn TF bundle and a 0.6 Volt-second OH coil. The PF system incorporates
passive stabilizers to support high elongation and beta. The power systems,
including a neutral beam, are drawn heavily from TFTR. The device will be
located in the former TFTR hot cell.
SST-1: An Overview (presented by S. P. Deshpande). The SST-1 is a
superconducting tokamak being designed at the Institute for Plasma Research,
India. SST-1 is a large aspect ratio tokamak, configured to run double-null,
diverted plasmas with significant elongation (1.7-1.9) and triangularity
(0.4-0.7). The major design parameters of SST-1 are major radius 1.1 m, minor
radius 0.2 m, toroidal field 3 T, and plasma current 0.2 MA. A pulse length of
1000 seconds in envisioned. The working gas will be mainly hydrogen. Both the
TF and poloidal field coils will be superconducting. The main current drive
will be from lower hybrid waves, while auxiliary heating will be done by ICRF
and neutral beams. The device is aimed at advanced plasma performance in
steady-state operation.
Present Status of JT-60SU Design (presented by G. Kurita). The JT-60
Super Upgrade Device is intended to establish an integrated scientific basis
for steady-state tokamak operation. Long pulse (1000-3600 seconds) operation
using full non-inductive current drive for 5-6 MA plasma current will be
investigated using ECCD (150-220 GHz) and NBCD (750 keV). Other major design
parameters of JT-60SU are major radius 4.8 m, minor radius 1.3 m, toroidal
field 6.25 T, elongation 1.8, and triangularity 0.4-0.8. The PF system
supports a symmetric double null for stability but a single null divertor is
planned for power and particle exhaust. Superconducting coils are used
throughout. Steady-state operational goals are bN ~ 3, H89P ~ 3, bootstrap fraction
~ 50%; although mainly deuterium operation is envisioned, these parameters
operated in an optional DT phase correspond to Q ~ 5.
Affordable Near-Term Burning Plasma Experiments (presented by D. Meade).
The thesis of this thought-provoking paper was that Fusion must succeed on its
own merits by competing economically with existing power producing technologies
rather than assuming the existing energy technologies will fail sometime in the
future. Such considerations imply that near-term burning plasma experiments
should certainly cost significantly less than $1B, preferably in the range 0.3
to 0.5 $B, if they are to be funded on a reasonable time scale. The paper
discusses various physics and technology approaches and advances that could
lead to staged burning plasma experiments that would allow progress even on the
above cost scale.
O4: Tritium Systems and Tritium Control, Alistair Bell (JET)
The papers in this session covered ITER tritium plant design, TFTR and JET
experience handling tritium in tokamak systems and the upgrading of the OMEGA
ICF target filling system.
Scott Willms of LANL opened with an invited talk on Tritium Processing for
ITER. He gave an overview of the current status of the design of the plant for
tritium recycling and process stream detritiation. The torus exhaust stream at
200 Pa-m3/sec could contain up to 2.5% organic impurities; the
performance of the impurity removal system is crucial. The options for tritium
recovery from impurities (Caprice, Electrolyser, Hitex, Palladium Membrane
Reactor, and Permcat) were described. All of these require a front end
permeator and evidence was presented that showed that the long term performance
of Pd/Ag permeators should be satisfactory. The optimisation of the Isotope
Separation System to reduce inventory and the characteristics of ZrCo storage
beds were discussed. A new proposal for the use of a polyamide gas separation
membrane to reduce the capacity needed for room ADS systems appeared
promising.
The second invited paper was given by Dennis Mueller on Tritium Retention and
Removal on TFTR. Extensive analysis and sampling during D-D operation had
shown that co-deposition with C was the main retention mechanism with 44% +/-
17% of the fuelled deuterium being retained. The results during each tritium
run period from 1993 to 1997 were consistent with this. Several clean-up
techniques had been tested and had been effective in removing about half of the
retained tritium. D2 soaking and N2 purging had been
shown to be ineffective, but D2 glow discharge cleaning, pulse
discharge cleaning and air purging were effective. The removal rate with He-O
GDC through the mechanism of carbon removal was slower but did not decrease
with time. Further work was proposed to be done on characterisation of carbon
dust and measurement of tritium levels.
Michael Kalish of PPPL presented an overview of the Operation of the TFTR
Tritium System. He described the process flows at TFTR including the addition
of the Tritium Purification System (TPS) which enabled tritium to be recycled.
In the four years of D-T operation, about 100 g of tritium was handled. The
low inventory TPS (1.4 g) became fully operational in February 1997 and 8 g was
processed before the TFTR shutdown. This enabled a significant reduction in
quantities both of the amount of tritium in molecular sieve beds shipped for
disposal off-site, only one being shipped during the TPS operational period,
and of LP18 supply containers, the rate decreasing from one per 2.5 days to one
per 12 days DT operation. The accounting system to meet the site inventory
limits was described including the arrangements for calibration.
The OMEGA laser facility the University of Rochester is being upgraded to use
cryogenic DT targets in 2000. The Omega cryogenic target system (OCTS) has
been designed to fill the plastic ICF targets at high pressure, cool them to
cryogenic temperatures and transport them to the target chamber. Art Nobile of
LANL gave a status report on some of the key design and safety issues of the
OCTS including the addition of three new glove boxes. Safety in the
compression of DT to 22500 psi for the permeation cell was an important
consideration. The site was licensed by the State of New York for 1 g of
tritium and releases of tritium had to meet a very stringent target of 200
mCi/y. Vacuum pumping had been optimised using a pumpdown code and pumps
carefully matched to the system requirements. Glovebox and target chamber
tritium removal systems were also discussed.
The latest results from tritium operation of the JET Active Gas Handling System
(AGHS) were presented by Alistair Bell. He summarised the commissioning tests
and the operation of the system supplying tritium to the JET torus. With 20 g
on site, about 55 g had been recycled during the current DTE1 experiments and
discharges to the environment had been well within the authorised limits. The
performance of the gas chromatography system, producing tritium with purity
better than 99.8% and of the cryodistillation system for clean-up of deuterium
to better than 1 ppm was summarised. The importance of the exhaust
detritiation system in minimising personnel doses during maintenance was
highlighted.
In discussions of the above papers, it became clear from the questions asked
that a key issue is tritium inventory and the related topic of turn-around time
of reprocessing. No serious technological problems were raised and safety
issues appeared to be managed satisfactorily.
O5: Plasma-Facing Component Technology, Ken Wilson (SNLL)
S. Chiocchio (ITER Joint Central Team) gave an invited talk on the "Status of
the Engineering Design of the ITER Divertor". The ITER steady state heat load
of 5 MW/m2 can be achieved with either detached or semi-detached
plasma operation, using a vertical target geometry. Significant progress was
reported for carbon fiber composite (CFC) and tungsten brush designs for the
divertor high heat flux components. Chiocchio concluded that the engineering
design for the divertor is at the level of detailed design definition to say
that it can fulfill the ITER requirements.
Progress by the U.S. ITER Home Team in the fabrication of
beryllium/copper-alloy and tungsten/copper-alloy high heat flux components was
described by C. Cadden (Sandia) in his invited talk "A Brief Review of Joining
Technologies for Actively Cooled Plasma Facing Components". Beryllium has been
successfully joined to copper with aluminum-based brazes that avoid the
transmutation issues of conventional silver-based brazes, and the formation of
brittle intermetallic phases between beryllium and most other elements.
Progress has also been made in joining tungsten brush structures to copper
alloy heat sink structures.
Three oral contributed talks also were presented in this session on
Plasma-Facing Component Technology. D. Driemeyer (Boeing) summarized the "ITER
Prototype Divertor Cassette Design, Manufacturing and Assembly Plans". By
manufacturing a full size, half-section of a prototype divertor cassette, the
ITER Home Teams are adding industrial considerations to the ITER design that
will improve both manufacturability and affordability. Technological
improvements like hot isostatic pressing of cast stainless steel components,
and welding using penetration enhancement compounds were given as examples of
improved manufacturability. M. Roccella (ENEA) described "Detailed
Electromagnetic Analyses of the ITER In-Vessel Components during Plasma
Disruptions." The three dimensional model for the in-vessel structures
contains over 50,000 elements. Roccella concluded that the most dangerous
disruptions were the fast centered disruptions for the shield blanket, and the
vertical displacement event (VDE) for the divertor. M. Lipa of the Tore Supra
Team concluded the session with his talk "Towards Long Pulse High Performance
Discharges in Tore Supra - Upgrading of Inner Vessel Components (Ciel
Project)". The Toroidal Pump Limiter (TPL) is being designed for 8
MW/m2 on the leading edge, and 5 MW/m2 on the flat high
heat flux tiles. The design uses carbon fiber composite tiles that are first
laser treated, and then joined to copper using active metal casting. The
assembly is then electron beam welded to the CuCrZr alloy heat sink. The high
heat flux testing and fatigue behavior has been completed. The TPL will be
commissioned in the year 2000.
O6: Heating and Current Drive Systems, Wally Baity (ORNL)
In the first paper, "Plasma Heating and Current Drive Systems for ITER
and Future Fusion Devices," J. Jacquinot set the stage for the rest of the
session by presenting the requirements, present status, and outstanding issues
of the four major auxiliary systems for ITER: NBI, ICRH, ECRH, and LHCD. The
functions of these systems are primarily to heat the plasma to ignition, to
provide plasma current for steady state operation, and secondarily to aid in
burn control, plasma rotation control, sawtooth suppression, and MHD island
control. Providing these functions will require multiple systems at a total
power of around 100 MW. Milestones have been met on critical components of the
NBI and RF systems, and research and development activities now should be
directed more toward testing complete prototypes.
- For negative-ion based neutral beam injection, deuterium at 1 MeV is needed
for central penetration of the ITER plasma. Three ports are envisioned for the
injection of 50 MW of beams to provide core heating, central current drive, and
plasma rotation. The beam parameters needed for ITER have been demonstrated
individually in development programs in France and Japan, but a full system
demonstration remains an issue. Additional issues are the large extension of
the nuclear confinement barrier volume and high cost.
- 50 MW of 40-70 MHz ICRH for second harmonic heating of tritium or minority
heating of 3He is planned, occupying four ports for the launchers.
The primary functions of the ICRH system are for localized heating, central
current drive, and some sawtooth suppression. The outstanding issues have to
do with the system response to varying load conditions, the high voltage
requirements, and the proximity of the antennas to the plasma.
- 170 GHz ECRH is expected to provide central heating and off-axis current
drive. Two ports are required for a total of 50 MW. Good progress toward
steady-state operation at high power has been achieved recently through the use
of a diamond window at the output of the gyrotron. Nevertheless, the slow
progress of this technology and high cost remain as issues.
- Finally, two launchers for a total of 50 MW of LHCD at 5 GHz would be needed
for off-axis current drive. Remaining issues are the H-mode threshold with
LHCD, the proximity of the launcher to the plasma edge, and the thermal and
mechanical loads on the launcher.
M. Kuriyama of JAERI reported recent results of the operation of the
negative-ion based NBI system on JT-60U. A total of 3.6 MW of deuterium at 350
keV has been achieved after 18 months of operation. The design goals for the
system include a beam energy of 500 keV, a total injected power of 10 MW, and a
pulse length of 10 s. The optimum source pressure was found to be 0.1 Pa,
considerably less than the design value of 0.3 Pa. The ratio of deuterium to
hydrogen ions was observed to be 70% at the same arc power. A source current
of 18.4 A of H- was obtained at 350 keV.
Y. Takeiri of NIFS described the status of the negative-ion based NBI for LHD.
Two beamlines providing 15 MW of 180 keV hydrogen for 10 s are under
construction with initial injection into LHD scheduled for September, 1998.
The source design parameters call for 40 A per source with 10 mrad divergence.
A development source at NIFS operated with 16.2 A of H-, with an
output vs. source power that did not appear to be saturated. Shaping of
electrodes to reduce electron acceleration was effective in increasing the
acceleration efficiency to 80%. A prototype LHD source is now in initial
operation. So far, 21 A of H- at 106 keV has been achieved in a
beam with a diameter of 24 cm.
R. I. Pinsker described a new matching circuit for one of the fast wave current
drive arrays on DIII-D which eliminates all tuning elements except for a
decoupler stub and provides good isolation of the transmitter from plasma load
changes. The system is pretuned for nominal plasma loading; other values of
antenna loading result in a portion of the transmitter power being diverted to
a dummy load. In the case of vacuum conditioning, about 80 percent of the
transmitter power is diverted to the dummy load, but the antenna can still be
conditioned to 30 kV with 1.1 MW from the transmitter. The antenna has been
operated into a DIII-D plasma with 95% of the transmitter power coupled to the
antenna. This method is optimal for a four-strap array fed by a single power
source with 90deg. phasing between adjacent elements.
R. W. Callis reported the status of the 110 GHz ECH systems on DIII-D. At
present there are two 1 MW gyrotrons in operation: one Gycom (Russian) unit
and one manufactured by CPI. The power output of the gyrotrons is limited by
their output windows. A second CPI gyrotron, scheduled for delivery in 1998,
is being fitted with a diamond window. Diamond windows represent a marked
improvement over existing designs. The launchers on DIII-D allow the ECH beams
to be steered poloidal over most of the plasma cross section at a fixed
toroidal angle to the magnetic axis. Central electron temperatures of 10 keV
have been obtained with about 1 MW of ECH power.
M. Lennholm reported recent improvements in the power handling and control of
the LHCD system on JET. Feedback control of the maximum electric field in the
waveguides is effective in preventing breakdown. The total power can be held
constant by independent control of the power output of the 24 500-kW, 3.7-GHz
klystrons. Feedback control of plasma parameters such as the internal
inductance and the reflection coefficient has also been implemented. The LHCD
system has been used to optimize the formation of reversed shear discharges.
Additionally, an ITER prototype hyperguide has been tested at 450 kW for 20
s.
O7: Plasma Control & Power Systems, Charles Neumeyer
(PPPL)
J. Wesley described the status of work to characterize ITER plasma disruptions
and consequences. Due to the large thermal and magnetic energy associated with
an ITER plasma, and the short time scale of disruption, the power levels are
impressive (Terawatt level for the thermal energy, Gigawatt level for the
magnetic energy). Runaway electrons are an area of concern (they can deposit
energy up to 100 MJ/m2), and more R&D in this area is
suggested.
P. L. Mondino provided an update on the status of the design and R&D of the
ITER power supply system. Levels of operation (600 MW grid power, 100 GJ
stored energy in the TF magnets, 60 kA steady state operation for the DC
circuits, 170 kA DC circuit breaking, 1 MV NBI, etc.) significantly exceed past
experience (on JET, TFTR, JT-60, etc.). Since many of the required
components exceed in rating what is available commercially at present, R&D
efforts have been undertaken and will be completed early in 1998. Results thus
far are very promising. Much work has been accomplished, and a design has been
developed for which there is a high level of confidence. The entire power
supply community will benefit from the developments of this work.
W. Reass described the design and installation of a 2-channel 10-MW amplifier
installed for MHD control on the Columbia University HBT-EP machine. The
amplifier is built around magnetically beamed triode tubes (600A/24kV/12kHz).
Thanks to the experience and creativity of the people involved, the complete
system was installed and commissioned in a short period of time at minimal
cost. With the likelihood of more smaller-scale alternative concept
experiments in the future, this mode of power supply work may become more
typical.
P. Sichta described the Digital Plasma Control System hardware and software
designed for TFTR. The hardware (VME based multi-processor system) was
originally procured for PBX, but was then used to replicate several of the real
time feedback control functions originally performed in analog fashion on TFTR.
A modern user interface was developed by which the operators can interact (set
parameters and view waveforms) via the WWW. Measured feedback loop performance
(timing) results were presented. The results of the work show that digital
technology is now powerful enough to execute real time plasma feedback
control.
O8: Inertial Fusion Engineering: Targets, Drivers and Chambers,
Grant Logan (LLNL)
Overall, the session reflected the need for innovation in inertial fusion
engineering, and it also reflected increased interest in laser-driven inertial
fusion energy (there were three papers on laser-driven IFE, and one on
heavy-ion driven IFE).
"Recent advances and challenges for diode-pumped solid-state lasers as an
IFE driver candidate (S. Payne, et.al.) -- Recent developments in four
areas have improved the candidacy of solid-state lasers for IFE: (1) lower
cost and more efficient laser-diode arrays for optical pumping, (2) development
of long-optical-storage-time media such as Ytterbium S-FAP crystals with
millisecond storage times, (3) gas-cooling of gain-media slab faces with low
beam distortion, and (4) annealing of neutron and gamma-induced transmission
losses in fused silica at high temperatures (~400 C). Principle
challenges remaining are the design and confirmation of direct-drive targets
with gains over 100, the development of adequate beam bandwidth and smoothing
required for high-gain targets, and the development of long-life chamber walls
with rapid clearing.
"Status of direct-drive laser-fusion target designs" (S. Bodner) --
Direct-drive IFE targets are simple and require modest intensity, but three
major problems must be overcome: (1) laser beam non-uniformities, (2) laser
plasma instabilities, and (3) hydrodynamic instabilities. Progress in recent
direct-drive target design address these concerns by adding incoherence to the
laser (trading-off focusability for uniformity), by using a sufficient number
of overlapping beams, and by preheating the target ablator to reduce
hydrodynamic growth rates. KrF lasers meet the laser bandwidth requirement,
but recent target calculations show that smaller solid-state laser bandwidths
may also work well enough.
"KrF lasers for inertial fusion energy" (J. Sethian) -- KrF lasers have
many desired features for direct-drive IFE: potentially low cost, short
wavelength, adequate beam smoothness, and a modular architecture. Major
development issues are: (1) rep-rate at high reliability, (2) durability of
the e-beam anode foils and optics, and (3) overall laser system efficiency with
gas recirculation. These development issues can be addressed with a modest
cost prototype test-bed operating at 5 Hz. Recent developments in pulsed power
solid-state switches with magnetic pulse compression may lead to durable pulsed
power in the $10/Joule range.
"Systems modeling for heavy-ion drivers" (W. R. Meier) -- There are a
variety of accelerator approaches for heavy-ion fusion to be explored with
comparative analysis for a given indirect-drive target requirement of beam
energy, pulse-shape, and illumination geometry. An integrated systems code
using MathCAD has been developed for such comparative analysis, which includes
self-consistent physics models, engineering constraints, and costs for all
subsystem components from the ion sources, through electrostatic and magnetic
transport, drift compression and final focusing to the target. The code has
evaluated a multi-beam linac baseline driver for a recent integrated 2-D target
design by Max Tabak, and will be applied to other accelerator approaches in the
future.
O9: Magnet Systems, Albe Dawson Larsen (MIT)
The session contained five papers, two of which dealt with ITER magnets, one of
which discussed the NSTX center stack design, and two of which presented
overviews of the KSTAR magnet system.
ITER and KSTAR are both tokamaks with completely superconductive coil sets.
The KSTAR machine should be constructed rapidly enough to provide valuable
input to ITER construction and operation plans. ITER is considerably larger
than KSTAR and has been in the engineering design phase for 5 years now,
following three years of conceptual design activities. KSTARUs design relies
heavily on work done for the aborted US TPX program. Of particular interest
from the ITER reports -- one an invited paper by Thome and Barabaschi for the
ITER team, and the other an in-depth discussion of alternative magnetic
configurations for plasma shaping by Mondini et al. -- was the decision
to change the PF design by increasing the number of PF coils and to
change all the PF coils to NbTi. This both reduces cost and simplifies
manufacturing, while maintaining the required physics parameters. The
Central Solenoid was reconfigured in one study, but the original
layer-wound single coil solenoid design was retained for the final
design report. It had the advantages of using TF forces to compress the
CS, and also for mechanical performance, whereas two of the alternative
designs could not satisfy mechanical design criteria.
Both the ITER CS and TF Model Coils under construction in the US and Japan, and
the EU and RF respectively, with support from all home teams for each, were
described and progress reported. Coil manufacture in Japan for the outer coil
and the US for the inner coil of the CSMC, is proceeding on schedule. The
inner coil will be delivered to the Japan Atomic Energy Research Institute in
July 1998 for installation and test at JAERIUs Naka facility. Japan and the US
have used different coil winding procedures, although both coils are Nb3Sn in
Incoloy 908 conduit. The TF coil will be delivered in 1999 for test in the
Karlsruhe Forschungszentrum test facility, using the Euratom LCT coil to
provide a 9 T background field. A TF insert coil that will reach the TF design
field of 13 T is also being fabricated. It will be tested in the bore of the
CSMC, to test conductor performance at its specified operational requirement.
The KSTAR PF and TF coil design was described in a paper by B. J. Lee et al.,
and the overall magnet system was described in a paper by J. H. Schultz et al.
All KSTAR coils, including up/down symmetric pairs of PF coils, the Central
Solenoid, 16 TF coils and the field error correction coils are
superconducting. The 16 D-shaped TF coils are the minimum number to produce
acceptable field ripple control while still maintaining access for tangential
neutral beam injection. All magnets are wound of cable-in-conduit conductor,
which is now a well-proven technology. The PF set allows for both steady-state
and pulsed ohmic operation. Details of coil design and mechanical support are
presented for all coil sets.
The National Spherical Torus Experiment (NSTX) has been designed, passed its
final design review, and is now under construction, with most components being
fabricated in industry. The Center Stack Assembly, the core of the machine, is
mechanically complex and has extremely tight tolerances. It consists of the
ohmic heating solenoid, the inner legs of the TF coils, three inner poloidal
field coils, thermal insulation, diagnostics and an elaborate support
structure. The paper describes the components, the R&D programs completed on
insulation performance and joint performance, the diagnostic systems, and
design, fabrication and assembly information on this extremely complex and
critical element of the NSTX. The assembly of the Central Stack will be
performed at PPPL, with the stack components assembled in an inverted
position. Once the stack is complete, it will be rotated 180{ and moved to the
operations hall or hot cell. The first plasma is planned for April 1999.
O10: Physics and Advanced Devices, V.S. Chan (GA)
This session covered the progress made in physics research and the applications
of physics understanding to the design of advanced fusion devices. Dr. M.
Zarnstorff (PPPL) gave a review of progress in transport barrier studies.
Transport barriers have been observed in a number of tokamaks and good
understanding has been achieved for ion heat and particle transport. He also
identified future research directions including producing transport barriers in
other configurations. Dr. R. Stambaugh (GA) reviewed the status of power and
particle exhaust research in tokamaks. Results from radiative divertors have
demonstrated the possibility to meet the ITER requirements. Discrepancy
however exists between the ITER methodology in calculating erosion and
experimental data. Dr. F. Najmabadi (UCSD) summarized the status of the ARIES
spherical tokamak power plant study. He emphasized the limited options for
current drive, the lack of confinement data and the divertor heat load as main
challenges. He also described innovations in center post design and liquid
breeder first wall blanket. Dr. W. Reiersen (PPPL) presented the design of the
Korean Superconducting Tokamak Advanced Research (KSTAR) device. The design
parameters, physics objectives and schedule were elaborated. Dr. N. Karulin
(ITER) highlighted simulation results of ITER advanced regimes using the ASTRA
code. He concluded based on his model that the Greenwald limit is not a
problem provided ITER operates at high beta. The final talk was by Dr. M. Peng
(ORNL) who discussed physics and system design for a spherical torus based
volumetric neutron source. He showed the latest START spherical tokamak result
from Culham with 30% volume averaged beta to substantiate the design physics
assumptions.
011: Next Generation ICF Devices,Carl Henning (LLNL)
This session covered the new laser fusion facilities under construction both in
France and the US. It was chaired by Dr. Carl Henning of Lawrence Livermore
Laboratory, who had guided much of the defining work on the National Ignition
Facility, and had coordinated the DOE approval process leading to the funding
decision.
The first paper on the Engineering Physics inside the LMJ Target Chamber was
presented by Dr. Daniel Schirmann of the French CEA. He focused on the design
of the reaction chamber and in particular on the coatings needed to prevent
ablation and damage to the first wall. Berylium carbide appeared to be the
best choice, but it needed to be coated onto an aluminum substrate. Schrapnel
could shock the surface and cause spallation of the vback. Thus, an aluminum
foam intermediate layer was being proposed by through a joint collaboration
with LLNL.
In the absence of Dr. Rick Sawiki, the second paper giving an overview of the
Engineering Challenges in the Design and Construction of the NIF Laser and
Target Systems was presented by Mr. Stan Sommers of the NIF Integration and
Analysis Team. The paper outlined the complexity of the facility for both the
1.8 megaJoule laser and the target chamber for which fusion ignition was
designed. The engineering phase is nearing completion and building
construction has begun.
In the third paper, Richard Foley filled in for Vic Karpenko to describe the
Design of the Target Area for the National Ignition Facility. The enormous
complexity of guiding 192 laser beams into the 10 meter diameter chamber,
together with diagnostics and a pellet positioner was evident. Like the
earlier French presentation on the LMJ, the favored first wall material was
beryllium carbide. It was to be coated onto tiles that could be serviced with
robotic manipulators. The chamber is presently being constructed of a 5083
aluminum alloy for low activation.
A fourth paper on the Stability Considerations in the Design of the National
Ignition Facility Target Area by Dave Trummer demonstrated the extensive
analysis necessary to achieve stable alignment of the laser beams with the
target. Ground vibrations were investigated as were thermal excursions and
wind induced deflections and vibrations of the building and laser structures.
By using the inertia and damping characteristics of the concrete building
together with the strength of the steel supports, it was possible to provide
adequate stability for the laser focus. Damped supports between the target
area floors and the target chamber were needed to achieve a stable chamber and
target pellet inserter.
The last paper was presented by Dr. Mark Rhodes on the Plasma Pockel Cell Based
Optical Switch for the National Ignition Faciltiy. He explained the basic
configuration and physics operation of these frequecy tripling optical cells
that are to convert one micron light into one-third micron light that better
couples to the NIF target to achieve ignition. The switch body has now been
changed to aluminum for better manufacturability and cost. A double cell
switch was sucessfully tested and a four cell NIF prototype is being prepared.
The switch has been designed for compactness to accommodate laser configuration
requirements.
O12: Data Acquisition and Diagnostics, Bill McHarg (GA)
This oral session was devoted to five papers related to plasma physics
diagnostics, to issues related to computer systems, and to remote
collaboration.
Sang Gon Lee, from the KBSI Institute in Korea gave a presentation on
"Diagnostics for the Korea Superconducting Tokamak Advanced Research (KSTAR)
Project". This talk was a summary of the diagnostics plans to be integrated
into the design of the KSTAR tokamak. Particular emphasis was being placed on
providing good diagnostic access for the tokamak.
"Design of a Ferroelectric Bolometer" was given by Marco Di Maio from the JET
Joint Undertaking. This talk discussed a new type of bolometer for measuring
the radiation output from a tokamak experiment. This new method should be
virtually immune to the type of noise encountered in a fusion experiment.
The paper, "Development of Improved Methods for Remote Access of DIII-D Data
and Data Analysis" was given by Kathy Greene from General Atomics. This talk
discussed how the "Ptdata" data access mechanism for DIII-D data is being
modified to improve data access over the wide area network. This modification
included a caching capability being built into Ptdata and also the use of
Distributed File System (DFS) disk systems.
An "Overview of the DIII-D Computer Systems" was presented by Bill McHarg. The
talk was an overview of all the different types of computer systems used in the
DIII-D environment, including UNIX systems such as SGI, DEC UNIX, HP-UX, SunOS,
Solaris, and Realix, as well as VAX-VMS and Alpha-VMS computers, all of which
are tied together by an ethernet-FDDI network. Different computer functions
were discussed along with future upgrade plans.
"Experiences with Remote Collaborations in Fusion Research" was given by Tom
Casper from LLNL. This paper discussed experiences over the past few years
with remote collaborations in the fusion community. These have included
PPPL-Wisconsin, LLNL-MIT, and LLNL-DIII-D. Some of the technologies used
(audio/video, DCE environment, interprocess communication, queueing system)
were discussed along with the future needs for remote collaboration.
P1: Magnet Systems - I, Joel Schultz (MIT)
Three subjects were covered in this session: the design of the SST-1
superconducting tokamak, improvements in the HT-7 superconducting tokamak, and
repair of a DIII-D ohmic heating coil lead.
The Indian Plasma Physics Institute in Gandhinagar is building a new tokamak
with NbTi, cable-in-conduit (CICC) superconducting TF and PF coils. The
tokamak also includes a set of normal copper OH initiation coils, vertical and
radial fast response coils, and in-vessel equilibrium coils. The TF support
includes an inner ring, outer ring, and side plates. The outer supports are
connected by shear keys, the inner supports by bolted teeth. The coil is
clamped to a ring with pinned cantilever connections, permitting radial motion,
to low heat-leak posts with intermediate nitrogen-cooled intercepts. The PF
coils achieve 6 T at 0.5 T/s. The conductors are 135 strand cables with 4.88
copper/noncopper ratio strands of 0.86 mm diameter. The superconducting
central solenoids are layer wound without joints. Terminations are soldered,
after spreading the final stage subcables into a flat blade.
The nitrogen shield of the HT-7 tokamak had to be redesigned when the number of
TF coils was reduced from 48 to 24 in order to permit larger auxiliary heating
ports. The shield, on both the inside and outside of the TF system, is
multipurpose -- reducing thermal radiation, slowing electromagnetic transients,
and helping to support the superconducting TF system. Radiation losses
increased by 25% because of the new ports, but were managed by subcooling the
nitrogen input and increasing the flow.
A 1995 leak in one of the DIII-D leads has reduced the capability of the
tokamak to 5 V-s. An in-situ repair is expected to increase the volt-second
swing to 7.5 V-s. The leak was caused by mechanical failure of a fiberglass
overwrap that hadn't been well impregnated. Since the leak was nearly
inaccessible at the bottom of the machine, special remote repair techniques
were developed using a prototype mockup. Long-handled tools, bore scopes and
dual TF monitors, remote tube cutting and soldering techniques were used. Each
piece of the clamp had to be slipped in individually, then assembled in-place
using the bore-scopes and monitors. The leak was bypassed by an internal
flow-through tube with expandable plugs on either side of the hole.
P2: Safety and Environment - I, Edward Cheng (TSI Research)
Nine papers were presented in this session. Six of them were devoted to
activation analysis for the International Thermonuclear Experimental Reactor
(ITER) and National Ignition Facility (NIF) design studies. The remaining
three papers were relevant to mobilization of plasma facing materials due to
plasma disruption and exposure to air and steam, and issues associated with
tokamak dust investigated for the ITER project.
The activation analysis performed for the ITER covers the following areas: (1)
N16 and N17 activity induced in the cooling water and the
consequences of these radionuclides present in the coolant loop as additional
sources of gamma heating and neutron activation; (2) Decay heat power profiles
based on a two-dimensional ITER neutronics model; and (3) Decay heat value in
the divertor dome component made of tungsten.
The decay heat value in the tungsten divertor plate is an important parameter
to estimate the temperature rise under any abnormal operating conditions.
Calculations performed by different groups using 1-D and 3-D Monte Carlo
methods showed a surprisingly good agreement when a similar heterogeneous model
taking into account the self-shielding effect is applied.
Calculations of prompt dose due to neutron streaming and experimental
verification of concrete activation due to 14-MeV neutrons were reported for
the NIF. It was concluded that the current NIF design and operational scenario
can satisfy the required biological dose limits imposed on the workers in the
control room and nearby areas. It was also experimentally found that ordinary
concrete is adequate without boron additives for the shielding purpose for the
NIF.
Disruption induced aerosol in accidental scenario of ITER was investigated
experimentally for copper, SS316, tungsten, and aluminum. Particle size
distributions were determined and reported.
Mobilization of various elements from austenitic stainless steels due to
intrusion in air or steam had been experimentally performed from 1983 to 1996
at the Idaho National Engineering and Environmental Laboratory. A compilation
of all data was presented including dose calculations resulting from the
updated database.
Tokamak dust, a dust mixture with radiological, chemically toxic, and
chemically reactive hazards, will exist inside the ITER vacuum vessel. An
overview was given on the dust safety limits, production, removal, and
surveying methods based on the investigation of three candidate ITER plasma
facing materials: beryllium, carbon, and tungsten.
P3: RF Heating and Current Drive Systems, Rich Callis (GA)
Fifteen papers were presented in this poster session, covering three different
frequency ranges for rf heating and current drive of plasmas. These were the
Ion Cyclotron range of frequencies (30 to 200 MHz), the lower Hybrid range of
frequencies (2 to 10 GHz), and the Electron Cyclotron range of frequencies (60
to 170 GHz).
Half of the papers addressed the topic of Ion Cyclotron Heating and
demonstrated that this technology is ready to support the future needs of
fusion, as well as present fusion experiments. Thomson Tube has developed a
new tube named a DIACRODE&tm;. This new structure overcomes the limits reached
by conventional tetrodes, and gives a neat solution to generate 2 MW cw with a
VSWR <= 2, any phase, for the new projects. Several papers by PPPL and
General Atomics covered the engineering solutions for the present generation 2
MW transmitters which operate in the 30 to 120 MHz range.
Tore Supra presented a paper on their ICRH antennas, which will aim at high
power operation of up to 25 MW with long pulse discharges (1000 s). To achieve
this challenging goal, some parts of the present antenna must be redesigned, in
particular, the lateral protections and the matching system. The Faraday
screen, with its actively cooled septum, and the current strap already fulfill
the new requirements. The vacuum feedthrough and the supporting structure need
a slight change of their cooling systems. The new ICRH antenna protection,
uses an upgraded technology based on Carbon Fiber Composite (CFC) shaped tiles,
intimately linked to the actively water cooled heat sink. The protection is
designed to withstand the nominal thermal load in steady state operation.
The papers on Electron Cyclotron Heating systems demonstrated that high power
>500 kW systems are now practical. Frascati Tokamak Upgrade (FTU), has four
ECRH systems at the frequency of 140 GHz and a total power of 1.6 MW for 0.5 s.
Each line transfers 450 kW of millimeter-wave power generated by a Gycom
gyrotron with an efficiency higher than 90%. General Atomics DIII-D tokamak
has two 110 GHz ECH systems nominally at 1 MW 1 to 2 second pulse length, and
JAERI is planning to install 4 MW of 110 GHz on JT-60U in the near future.
Only one paper covered the Lower Hybrid Technology. This was a paper
describing a conceptual design of a LHW system for the ITER EDA The novel
concept is based on the passive active multijunction (PAM) which associates a
good coupling of the slow wave with an efficient cooling of the grill mouth.
The PAM is fed by an oversized section (hyperguide) excited by several mode
converters which ensure poloidal sharing of the RF power. The 50 MW of power
required to cover the envisioned scenarios can be coupled by two launchers
located in two ports of the machine. The working incident power density is 23
MW/m2 which is routinely achieved in present experiments at 3.7 GHz.
The launched N|| spectrum of the wave centered at N|| =
2, is produced by a PAM made of 29 passive waveguides (WG) and 28 active WG
with a 270 deg. phasing between adjacent WG. The passive WG facing the plasma
are Be coated (or, alternatively, CFC brazed on) DS copper and actively
cooled.
P4: Divertor and Plasma-Facing Component Engineering, Dan Driemeyer
(Boeing)
The sessesion was well-attended with over 100 people visiting to review the
displays and question the presenters. Posters that generated particular
interest included the following:
- A report on the development of measurement techniques and installation
procedures to install and accurately align the new, W-shaped divertor in
JT-60U.
- A report on the degredation of plasma facing materials when subjected to
disruption-like thermal shocks.
- A report on the fabrication and testing of new Be/Cu thermal fatigue mockups
in the EU which showed that a silver-free CuMnSeCe braze process can now meet
the ITER requirements.
- A report on the initial-phase fabrication and installation of the D-III
radiative divertor, including innovative manufacturing development work with
vanadium on the inner backing plate hardware.
- A report on the fabrication and testing of small-scale and large-scale (1.3-m
long) ITER target plate mockups in Japan, which demonstrated that the ITER
requirements can be met on full-scale hardware using silver-brazed UD-CFC
saddle tiles. This paper also described testing of 5 mm thick CVD-tungsten
layers that show promise.
- A report on assessments of structural attachment concepts for the ITER PFCs
which shows a promising alternative using simple expanded hollow copper pins.
P5: Data Acquisition and Diagnostics, Paul Sichta
(PPPL)
Nine posters were presented at this session. Seven addressed data acquisition
systems and four described diagnostics. The posters described accomplishments
and upgrades for the tokamaks DIII-D, TFTR, TEXTOR, and JT-60U.
The data acquisition portion of the session was dominated by General Atomics
(GA). They described upgrades to the DIII-D neutral beam computer controls in
the areas of operations, hardware, and software. A poster presented by B. G.
Penaflor (GA) addressed long-term software maintenance. As experienced in
other mature tokamaks, maintenance can become significant if the individual
designs do not encourage project-wide structure and style.
M. Korten presented an upgrade to the data acquisition and control systems for
TEXTOR-94. The system design used modern communication technologies such as
FDDI and the Grand Interconnect (Kinetic Systems Corp.). Modern hardware also
was used, such as Alpha (Digital Equipment Corp.) technology and VME field I/O.
Both the DIII-D and TEXTOR upgrades provided system control via a standard
TCP/IP network. This architecture will become common as remote control rooms
gain acceptance and collaborations between fusion facilities grow.
The mechanical installation of TFTR's Poloidal Rotation diagnostic was
presented by L. Dudek (PPPL). The installation of this diagnostic required a
post-DT vessel opening to install the diagnostic's shutter/window assembly.
The diagnostic's optics were precisely aligned using external reference points
and mechanical sightlines. This was an example of how creative engineering
solutions can be used to implement upgrades and repairs on a DT-activated
machine.
A proposed upgrade of the DIII-D Thomson Scattering diagnostic was presented by
D. G. Nilson (LLNL). The proposal would extend the present scattering
diagnostic's viewing region inboard to provide the capability to diagnose
shearing phenomena in the plasma core.
Two posters addressed the measurement of magnetic fields. P. Fiorentin
presented results from evaluation of a protoype Stationary Induction Field
Sensor. A key feature was the use of ball bearings to reduce field measurement
errors due to friction. K. Kurihara (JAERI) presented a high-precision digital
integrator for use in measuring magnetic fields. He described three versions
of the integrator circuits, explaining the problems resolved by each (new)
model. This integrator is used on JT-60U and was shown to be accurate enough
for ITER-like (steady-state) applications.
P6: Magnet Systems II, Joseph V. Minervini (MIT)
Nine posters focused on various aspects of magnet systems, both conventional
and superconducting, were presented in this session. More than half the papers
reported work on the International Thermonuclear Experimental Reactor (ITER),
two papers on TEXTOR-94, one on Alcator C-MOD, and one on current imbalance in
superconducting cables.
Three of the ITER papers described work done on alternative poloidal field coil
configurations. Work by Bulmer and Neilson reported on two configurations for
the Central Solenoid (CS), one RSegmentedS design with all pancake windings,
and a second RHybridS configuration which has a layer-wound central module and
pancake-wound end-modules. The Segmented Design had superior plasma
performance but resulted in magnetic fields at the winding joints too high to
be practical. The Hybrid design also gives improved performance over the
baseline design, but with excessive insulation shear stresses, perhaps
resolvable with proper R&D.
Heitzenroeder presented an overview of the Hybrid CS design for ITER. The
shortened length of the main module allows for a pair of discrete coils above
and below the TF coils. This reduces the fields at the PF2 and PF7 coils
allowing them to be made with NbTi at reduced cost and complexity.
The paper presented by Krivchenko gave the 2D and 3D global structural analysis
of the ITER reference CS coil design in comparison with the Hybrid CS design.
The reference design was preferable because of acceptable stress levels,
whereas the Hybrid alternative suffered from higher insulation shear stresses
and increased TF bending stresses.
Details of the ITER CS insulation shear stresses were summarized by Titus. The
result was that a portion of the CS coil violated the design criteria for the
preferred Kapton-Prepreg insulation system. This may be resolved with more R&D
of plasma etched Kapton tapes as the insulator.
The last ITER paper dealt with the design criteria for the fast discharge
system required in case of a quench of one or more PF or TF superconducting
magnets. A significant result is that the presence of a short circuit in one
TF coil section during fast discharge could lead to large overcurrent and
thermal heating of the shorted section.
Two papers dealt with the design of a proposed Dynamic Ergodic Divertor for the
TEXTOR-94 tokamak. Giesen described the design of the multipolar helical coil
system which generates a 4-phase rotating field. It is comprised of 16 helical
plus 2 stray field coils mounted on the inboard side of the vacuum vessel
where they must operate at 2500C. Descriptions of the coil design, cooling,
in-vessel components and power supply systems were given. A paper presented by
Neubauer presented the coupled resonant compensation circuits which must be
designed to account for the residual non-symmetric effects.
Myatt presented a 3D coupled electromagnetic-thermal analysis of the current
diffusion in the finger joints of the Alcator C-MOD TF coils. A 3D ANSYS model
with sub-modeling was used to evaluate the peak temperature magnitude and
location in the felt metal sliding finger joints, including effects of
time-dependent current diffusion and locally damaged felt metal. The
conclusion was that the temperature increase due to damage was modest and not a
problem.
A paper presented by Nomura described an experiment to used to investigate the
current imbalance and correction methods in multistrand superconducting cables
which may cause premature quench of the coil. The work highlighted the effects
on current distribution of leakage inductance and contact resistance among the
cable strands. Experiments performed on a High Temperature Superconducting
(HTS) tape showed that contact resistance or use of an iron core current
balancer were effective in reducing imbalances at commercial frequencies.
P7: Nuclear Engineering, Mohamed Sawan (UW)
A paper titled "Effects of Resonance Absorption in Fusion Device Heterogeneous
Media" was presented by J-Ch. Sublet from UKAEA Fusion. This paper addressed
the self-shielding problem associated with the giant resonances in the tungsten
absorption cross sections. It was shown that proper calculation of the
tungsten decay heat in the ITER divertor requires accurate three-dimensional
modeling of the heterogeneous geometry and use of continuous energy cross
sections in the transport calculation, along with effective cross section
corrections in the activation calculation.
M. E. Sawan from the University of Wisconsin presented a paper titled "Nuclear
Heating and Damage Profiles in the ITER Divertor Cassette". This paper
discussed the three-dimensional neutronics calculations performed to determine
the detailed spatial distribution of the nuclear parameters in the divertor
cassettes used in ITER. These parameters included power density, atomic
displacement and helium production. The largest heating and damage occurs in
the dome which has full view of the plasma. The total nuclear heating in the
60 divertor cassettes is 101.6 MW.
A paper titled "Three-Dimensional Analysis of Nuclear Heating in the
Superconducting Magnet System in ITER due to 16N Gamma-Rays in the
ITER Shielding Blanket Water Cooling System" was presented by H. Iida from the
ITER JCT. In this paper, results of detailed 3-D Monte Carlo calculations that
determine nuclear heating resulting from activated water are described. The
total g-ray energy emitted by the decay of
16N in the cryostat
is about 50 kW with 1.1 kW of it being deposited in the cryogenic temperature
components. Results showed that an additional guard pipe around the cooling
pipes is not required.
R.J. Cerbone from TSI Research presented a paper titled "Neutronics Analysis of
a Spherical Torus Based Volumetric Neutron Source". In this paper, the results
of neutronics calculations for a ST-VNS with neutron wall loading ranging from
0.5 to 5 MW/m2 were discussed. Analyses have been performed for
several designs to determine the sensitivity of the system performance to
variations in aspect ratio, elongation and fusion power. Neutronics
calculations also were carried out for the blanket and divertor materials
presently assumed in ITER.
A paper titled "Measurement of Radioactivity in Mixed D-T and D-D Neutron Field
at TFTR" was presented by H.W. Kugel from PPPL. A large number of capsules of
materials of direct relevance to fusion power development were irradiated for
various neutron fluences at locations close to and around the TFTR vacuum
vessel. Measurements of decay radioactivity of various samples have led to a
database of saturation activities for radioactive products resulting from a
large number of neutron-induced reactions for various neutron energy spectra.
P8: Materials Engineering, Panos Karditsas (UKAEA)
Three papers dealt with the potential use of zirconium alloys in fusion, a new
method of production of the ITER Glidcop Al-25 first wall plates and modelling
of a cylindrical Inertial Electrostatic Confinement (IEC) fusion device.
For forty years, zirconium alloys have been a mainstay material for fuel
element cladding and pressure tubing for a number of thermal reactor concepts.
Whilst fully adopted in LWR and HWR units, zirconium alloys have not been
employed in fast reactors, nor do they seem to have been seriously considered
for future fusion power plants. The lack of interest from the fast reactor
community stems from the unsuitability of zirconium-based material to
accommodate the high power core density, high temperatures and need for liquid
metal coolants thought necessary in all current designs. Fusion, in contrast,
contemplates some concepts that require pressurised water cooling for the
blanket and divertor.
Zirconium and certain of its alloys have the following features that make them
attractive in nuclear applications:
1. Low absorption cross section for thermal neutrons.
2. Very corrosion resistant in aqueous and air environments.
3. Favorable mechanical properties at temperatures typical of pressurised
water-cooled systems.
4. Good fabrication and joining capabilities.
The principal alloys used in nuclear applications are the zircaloys 2 & 4,
and the binary Zr-Nb alloy. The properties of zirconium and Zr-alloys have
been reviewed in light of forty years of accumulated fission reactor
experience. Zr-based materials apparently have a good combination of
properties that makes them potentially attractive for some fusion uses. On
limited analysis, it would appear that corrosion, hydride formation and
activation characteristics do not bar Zr-alloys from use in near-term
fusion power plants (including possibly ITER). However, there are still doubts
over the lifetime performance of zircaloy under combined creep, fatigue and
irradiation conditions typical of the first wall of a commercial fusion power
plant. It is recommended that further exploratory work be undertaken and that
the fusion community should be asked to comment on the potential viability of
zirconium based materials.
Glidcop (copper which is dispersion strengthened with aluminium oxide) is the
primary candidate for ITER applications requiring copper alloys, including the
first wall and divertor. The material and plate properties using the IG1
process were compared to the IG0 process. In the IG0 specification, the plates
are made by first decladding the extruded plate to remove the remnant copper
vessel used to contain the power during extrusion, then are cross-rolled to net
1 m width, then straight-rolled to the final thickness and length, and then are
annealed at 1000 C to simulate the hot isostatic pressing process during first
wall module fabrication. The IG1 specification was developed for full
production plates for first wall module fabrication. The production sequence
for the plates is the same as in the IG0 specification, with the exception that
the plates are supplied clad and are not annealed. The copper cladding is left
on the plates to protect the core Glidcop material from oxidation and damage
during rolling and handling. The separate annealing process is eliminated
because the plates will undergo a ~1000 C heating during hot isostatic pressing
during assembly. The elimination of the unnecessary production steps is also
expected to reduce the manufacturing cost of the plates for the ITER program.
The general conclusion was that, to within experimental measurement errors, the
mechanical properties of the plates were the same.
A model for an Inertial Electrostatic Confinement (IEC) cylindrical fusion
device was presented, to understand the fundamental physics and predict
parameters of interest. An experimental device is in operation at the U. of
Illinois (Urbana-Champaign) with deuterium gas. The machine has a working
range of 0.1-0.44 Pa gas pressure, neutral gas temperature 300-500 K, electrode
current 10-40 mA and cathode voltage 10-30 kV. The device is capable of
generating neutrons at a rate of 2x105 n/s at 30 kV and 40 mA.
There are two modes of operation. The beam-beam mode, where counter-beam
streaming ions produce neutrons, and the beam-background mode, where the beam
interacts with the background gas in the chamber to produce neutrons.
Conservative scaling laws are used, based on the experimental results of the
beam-background neutron generation mode only, to predict that neutron
generation rates of the order of 108 n/s can be achieved with a
variety of voltages and currents ranging from 40 kV/10 A to 80 kV/1 A. Larger
devices are theoretically predicted to be capable of producing up to
1010 n/s at 100 kV and 100 A.
P9: Tritium Systems, Dennis Mueller (PPPL)
Eight posters were on display in this session. The topics ranged from tritium
control during vacuum vessel vents to the design of tritium systems for ITER
and inertial fusion target fabrication.
Blanchard reported on the use of a flow-through system with a bubbler to trap
tritium used on TFTR during vessel vents that minimized personnel exposure.
Two papers focused on the use of Palladium permeators or reactors to separate
hydrogen isotopes from impurities and a third found permeators a possible
choice to separate hydrogen from inert gasses. Two papers expressed concern
about effectiveness of the permeators at low partial pressures of hydrogenic
isotopes and called for research to study their effectiveness under these
conditions, the other, by Honnel, reported on measurements at low partial
pressures. Honnel et al. found that, at least for protium, permeators can
reduce the concentration of hydrogen by over four orders of magnitude even in
dilute streams (<1% H2). Willms reported on the adsorption of
hydrogen isotopes on molecular sieve at liquid nitrogen temperature and found
that T2 had the highest loading for a given partial pressure.
Wermer et al. described the successful use of a Zr2Fe metal hydride
getter to clean up tritium from a helium glovebox. The design of the OMEGA
target system was reported by Goodin. The prototype testing has resulted in
simplification of the system's design. This should permit easier maintenance
and better reliability. A surprising result was reported by Sherman et al. in
regard to the radiochemical reactions between tritium and air. They found as
yet unexplained changes in the tritium and oxygen content of a tritiated air
sample. The T2 and O2 partial pressures decreased as
tritiated water was produced, but not in the expected 2:1 ratio and
T2 continued to decrease even after the O2 had
disappeared, but at a slower rate. There was no HT produced that would account
for the disappearance of T2. The processes involved remain
unclear.
P10: Vacuum Systems, Michael R. Kalish (PPPL)
Four papers were presented in this poster session. Two of these papers were
related to R&D efforts for ITER, the third described the ITER cryopump
design, and the fourth was an overview of the KSTAR Vacuum Pumping System.
A paper entitled "The Influence of Long Term Exposition in Tritium on Vacuum
and Physical Characteristics of ITER Cryosorption Panel Mock-Ups" was presented
by N. Kazakovsky. The results of actual tests on ITER cryopanel material were
presented. The samples were exposed to tritium, thermally cycled, and tested
for changes in their physical properties such as microhardness. Tests also
were done to determine the residual tritium after bake out. These data are
important due to issues regarding high residual tritium inventory of the cryo
panels during ITER operations.
"Pumping Speed and Selectivity Phenomena for Cryopumping of ITER Relevant
Exhaust Gas Mixtures" was presented by Chr. Day and Schwenk-Ferrero. This
paper also was a presentation of results from testing designed to provide data
for ITER cryopump design. A cryopanel comparable to the design foreseen for
ITER's primary cryopump was used to examine desorption characteristics and
pumping speeds as well as the effect of poisoning on pumping performance. The
paper discusses how the combination of sorption and condensation effect the
selectivity for gas species. Also examined is the optimization of pump
geometry and its effect on selectivity.
The next paper, "Detailed design of the ITER primary cryopump model" by N.
Petersohn, describes the design of a scale prototype of one of the 16 primary
cryopumps planned for ITER. The surface of the cryosorption material was
designed at 1/2 scale to provide a pumping speed of 41.5 m3/sec.
The scaled down design is meant to prove out the concept and examine
operational behavior. Additional studies will be necessary to examine areas
such as thermal loads on shields during regeneration and valve actuator
techniques.
The last paper presented "The Integrated KSTAR Vacuum Pumping System",
J.Y.Lim, provides an overview of the KSTAR vacuum pumping requirements and
design. The system will provide base partial pressures of <
1x10-7 torr for fuel gases and < 1x10-9 torr for
impurities. The paper discusses the analysis which led to the final
configuration of the vacuum pumping geometry. Also the various pumping
subsystems, Torus, Cryostat, and Foreline and Roughing Pumping Systems are
presented along with a schematic diagram summarizing the systems.
P11: Plasma-Material Interactions and In-Vessel Tritium Control,
Yoshi Hirooka (UCSD)
Presented in this session were 12 papers: 7 from the US, 4 from Russia
and 1 from Germany. This clearly shows a strong commitment of Russian
scientists in this area of research.
Burtseva (Efremov Institute) presented two papers: one on the neutron
radiation effect on thermal conductivity and the other on deuterium retention.
The materials evaluated in these papers are Ti-doped and B-doped graphites.
Results clearly indicate the benefit of these dopants, but there is no
explanation given as to why doping works so well.
Two papers brought from PPPL both concerned techniques for lithium coating for
wall conditioning. Kugel reported on the successful use of an ordinary
evaporation source for lithium wall conditioning. On the other hand, Labik
presented a rather exotic method, using AC shots of a high-power laser to melt
and splash lithium so that a large quantity of will be injected during
discharges -- a method called DOLLOP (Deposition of Lithium by Laser Outside of
Plasma).
Nornoo and King (University of Houston) reported on a new method of simulating
disruption conditions using an electromagnetic railgun and the initial results
on experiments and modeling analysis. The UCSD-PISCES team reported on recent
measurements on beryllium erosion by deuterium plasma and deuterium retention
and the effect of surface temperature.
Opimach (TRINITI) presented a paper on the high heat flux test and subsequent
deuterium retention measurements on a Russian B4C-coated graphite
using the DIMES facility in DIII-D. Mallener (Jülich) reported on the
preparation and subsequent high heat flux tests on plasma-sprayed
B4C on stainless steel for Wendelstein-X and tungsten on copper for
ITER. A series of publications on B-doped and B4C-coated graphites
shows strong interest in boron application in fusion from both Russia and
Europe, which has never been a high priority in the US.
Two more papers from PPPL were presented on tritium removal. Nagy reported on
TFTR's experience on tritium removal and reviewed a variety of methods,
including simple glow discharge, He+O glow, air venting with the wall at baking
temperatures, etc. Skinner reported a new method of tritium removal, using
laser to induce thermal desorption of tritium. Information of this kind will
be useful for future DT-burning fusion experiments, including ITER. A modeling
paper on tritium inventory was reported by Kuan from UCLA with the emphasis on
the effect of codeposition but the method of estimating the total erosion
appears to need an improvement.
The last paper in this session was presented by Belyakov (Efremov Institute),
who reviewed recent efforts on ITER divertor component design, mock-up
fabrication and related technologies such as brazing.
P12: Safety & Environment II, Neill P. Taylor (UKAEA)
Safety analyses of ITER and of conceptual fusion power plant designs, together
with some related experiments, were the subject of the eight poster
presentations in this session. Sophisticated computer codes are used for
thermal-hydraulic, aerosol, and accident consequence calculations. Two papers
were concerned with the application of these to assessing the outcome of
postulated loss of coolant accidents (LOCAs) in ITER, and a third performed
analysis to predict peak temperatures in the ARIES-RS tokamak power plant
following a LOCA. The ITER analyses showed that safety features are successful
in mitigating the effects of the in- and ex-vessel LOCAs, while the ARIES
analysis showed that moderately high peak temperatures might be reached in
first wall structures of power plants.
The codes used for such analyses need validation, especially in the context of
ITER licensing, and this was addressed by a paper which compared
thermal-hydraulic code predictions with the results of tests in which high
pressure high temperature water was discharged into a vacuum to impinge a
well-instrumented target. Another paper outlined a new analytical technique
for inverse heat transfer, using Laplace transforms.
A further ITER safety analysis modeled the accumulation of hydrogen gas at the
ceiling of a room in the tritium plant, during an accidental jet release of a
hydrogen isotope from a process line. The calculations showed that ignition of
the detonable cloud would produce a peak overpressure within the design
pressure limit for the room.
One safety concern is the potential for chemical reactions of beryllium with
steam, producing hydrogen. The available surface area of beryllium is an
important parameter in predicting the reaction rate, and one paper reported the
results of BET surface area measurements of a number of materials including
consolidated and plasma-sprayed beryllium. For the plasma-sprayed samples, an
important observation was a large proportion of the porosity which is closed in
94% T.D. dense deposits becomes open at 92% T.D.
A pellet-injection scheme for a Fast Plasma Shutdown System for ITER was
proposed in a paper which showed that carbon or beryllium pellets propelled by
high pressure helium gas, normally isolated by an electrostatic valve, could
provide satisfactory shutdown performance.
P13: Plasma Facing Components Engineering, Richard Nygren
(SNLA)
In their paper, "Development of Tungsten Brush Structures for PFC Armor
Applications," K. Slattery et al. described a method for fabricating
"brush-like" structures (clusters of small filaments or rods) for armor in
plasma facing components as a means of reducing thermal stresses at the joint
with the heat sink. Methods under development use 1.6-mm and 3.2-mm-diameter
tungsten welding electrodes as stock for the armor and welded metallic
honeycomb for fixturing during application of the copper backing matrix. In
one technique, Cu or functionally-graded Cu/W are plasma sprayed to the rear
surface of the fixtured W brush armor. Other methods include casting of the Cu
bed and diffusion bonding of the rods through a HIP or hot pressing process
that forces the rods into the Cu bed. The copper bed of the brush can then be
joined to a Cu-alloy heat sink using low temperature (below 550 C) diffusion
bonding techniques.
In "Melt Layer Erosion and Resolidification of Metallic Plasma Facing
Components," G. Dale and M. Bourham describe experiments using an
electro-thermal gun PIPE to simulate material ablation and the resolidification
of melted material that results from a plasma disruption or from electric
launch devices. A tokamak disruption may impart 10 to 100 MJ/m2 or
higher to the first wall in 0.1 to 1 ms and electrically driven launchers can
impart between 10 to 12 MJ/m2 in 0.1 to 5 ms. PIPE produces a high
density (1025 to 1026 1/m3) low temperature (1
to 3 eV) plasma for pulse lengths greater than 100 ms. They are studying 306
SS, OFHC, and Al. The resolidified material has a different grain structure
than the unaffected material. The resolidified thickness varies from less
than 10 mm to greater than 100 mm.
In "Compliant Layer Bonding of Be to Cu for Use in Plasma Facing Components,"
C. Cadden et al. describe recent progress in joining Be plasma facing
armor to copper alloy heat sinks. Joining techniques with various interlayers
have been explored to prevent formation of deleterious intermetallic compounds
at the bond line and to reduce differential thermal expansion stresses. Be
components require careful handling to prevent the formation of a tenacious
surface oxide which subsequently inhibits metallurgical bonding. Relatively
thick layers of Al, which does not form intermetallic compounds with Be, and
thin titanium layers (diffusion barriers) were among the materials used. An
Al-Si braze alloy was used to join S-65C beryllium to the aluminum surface of
an explosion bonded Al/Ti/Cu plate to produce a structure with reasonable
integrity at temperatures of 20 and 300 C and considerable ductility.
The strengths of samples is comparable to that of the Al layer. Using
AlBeMet-150&tm; (a Be alloy with ~45 w/o Al) rather than Al in the explosion
bonded configuration improved bond strength with no loss in chemical stability.
In "A Comparison of Stresses in Armor Joints With and Without Interlayers," R.
Nygren summarized analytical results on compliant interlayers between W armor
and a CuCrZr heat sink. The 2-D analyses were done in PATRAN/ABAQUS with
generalized plane strain elements, temperature dependent material properties
and (kinematic) strain hardening. The thermal history began with fabrication
(stress free state) at 550 C followed by cooling to 25 C and a heat flux of 5
MW/m2. The W50-Cu50 interlayer (a hypothetical material) had very
little plastic strain but high residual stresses. Both the no interlayer and
the W-50-Cu50 interlayer cases exhibited high (~ -390 MPa) X stresses (parallel
to joint) in the armor at the center of sample and high Y stresses near the
edge of the joint. In comparison, the X and Y residual stresses with the 1-mm
soft copper interlayer were roughly half the values of those without the
interlayer. Both the continuing plastic strain with thermal cycling in the Cu
interlayer and the presence of high residual stresses (but relatively little
plastic strain) with the stronger W50-C50 interlayer make fatigue a concern
during operation.
In "Steady-State Impurity Control by Gettered Moving-Belt Plasma-Facing
Components," Y. Hirooka et al. revisit a novel concept with a moving
belt that continuously resupplies a getter coating while removing heat and
carrying embedded tritium and impurities to a handling site away from the
immediate area of the plasma edge. To minimize complicated MHD effects
(associated with an earlier concept with metal belts by Snead and Vesey),
semi-metals or semi-conductor materials such as C-C or SiC-SiC composites are
proposed for the moving belt. Li, Be and B are considered for the getter. The
heat removal can be done either radiatively or by contact with a heat sink,
depending on the heat loading condition. The paper shows a concept with
successive stages for tritium recovery, heat removal and getter coating along
with calculations to substantiate the sizing of the components and feasibility
of the technology.
In "Development of Tungsten Coatings for ITER Divertor Components," Riccardi
et al. describe the EU design of the ITER Divertor Wing and,
specifically, a process for plasma spraying 5 mm of W armor (low sputtering
rate) on the wing. The aim is to qualify a plasma spray process that can
reliably produce up to 5 mm W coatings on CuCrZr tubes. The armor must
withstand thermal fatigue under heat fluxes up to 5 MW/m2. Low and
high pressure plasma spray processes have been studied and the selection of the
bonding interlayer was crucial in order to get good adhesion of the coating to
the CuCrZr substrate. Al-12Si and Ni-20Al, which are more creep resistant than
pure Al, were used. Electron beam thermal fatigue tests were performed at
CEA-Framatome-Francia. The mock up with 5 mm armor done with low P technique
survived without any damage to a record 1000 cycles at 2 MW/m2 and
200 cycles at 4 MW/m2.
P-14: Electromagnetics and Electromechanics, Peter Titus (MIT)
Most papers in this session addressed vessel loading of vacuum vessels
resulting from disruptions. One paper reported the results of using a
ferromagnetic vacuum vessel.
"Transient Behaviour of the Ignitor Plasma Chamber Under Vertical
Displacement and Halo Current Event", by G. Mazzone, A. Pizzuto. Loads on
the vacuum vessel were computed based on a vertical disruption preceding
development of halo currents which were then assumed to be 25% of the initial
plasma current with a peaking factor of 2. The dynamic load history was then
applied to a dynamic structural model. Elastic- plastic material properties
were used in which strain rate effects were included. Plastic strains were
then compared with ASME III criteria to show adequacy of the vessel.
"Assessment on Electromagnetic Force Reduction on Modular Type Blanket
Structure at Plasma Disruption for the ITER", K. Kitamura, et.al.
Electromagnetic and structural analyses were performed on an inner wall
blanket module. The addition of toroidal slits reduces eddy current loads and
attachment to the backing plate. Eddy currents were computed using the EDDYCAL
code. Force reductions of up to 25% and stress reductions of up to 22% are
cited for the addition of 3 slits.
"Discharge and Poloidal Magnetic Field Reconstruction in a Ferritic First
Wall Tokamak", M. Abe, T. Nakayama. Use of F82H ferritic steel for a
vacuum vessel is investigated. It has low activation characteristics, and is
less expensive than stainless steel. Experiments in the HT-2 tokamak showed
acceptable vacuum performance. Plates of the ferritic material were inserted
into the existing stainless steel vessel of the HT-2 tokamak. Magnetic
properties of the vessel were shown to have an acceptable effect on the plasma
discharge.
"The Relation Between Halo Currents and Plasma Displacement/Deformation in
JET", P. Andrew, P. Noll, V. Riccardo. Halo current magnitudes and
distributions are investigated. Instrumentation used to measure halo currents
is described. Halo current magnitudes are related to the plasma current
vertical moment. local halo current magnitudes are related to plasma vertical
force balance and an effective width of the current path.
"Asymmetric Vertical Displacement Events at JET", V. Riccardo, A. Kaye, P.
Noll, T. Raimondi. The upper boundary of the vessel sideways displacement
is observed to scale with the product of the plasma current and toroidal field.
This maximum is achieved when the plasma kinks at its full current and the kink
lasts long enough to produce a sufficient impulse to overcome the inertia of
the vessel and the magnetic damping of the vessel motion. Higher poloidal
modes are postulated as the cause for some of the observed distributions of
halo and toroidal currents. Analytic expressions are provided for the force
distribution on the vessel, and a simple dynamic simulation is presented which
predicts net displacements and the effects of magnetic damping and stiffness of
restraints that have been added to the JET vessel. The paper concludes that
large tokamaks must account for these lateral forces on the vessel or provide
means to mitigate the effects of the asymmetric disruption.
P 15: Assembly, Fabrication and Maintenance, Gerald W. Wille
(Boeing)
Sixteen papers describing fabrication, assembly, and maintenance of ITER and
JET were presented. The session was well attended by over 100 people and very
informative on the latest status of items related to these machines. Three
papers described remote metrology of structures using coherent laser radar
(CLR) and digital photogrammetry methods. Preparation for fully remote
replacement of 144 JET divertor modules and the operator interfaces with the
remote handling equipment were described in two papers. Remote handling for
ITER was reported in five papers. These covered blanket coolant pipe
connections; tests and full-scale development of equipment for blanket modules;
divertor maintenance; and guidance, navigation and docking of transport casks
for components. Four papers presented the progress on ITER fabrication and
development for cassette body, dome, middle-scaled shielding blanket module,
and a completed full scale sector model of the vacuum vessel. The overall
assembly plans for ITER, including tolerance concerns, tooling, and welding
were described in one paper.
P16: Plasma Control and Control Systems, Robert Woolley
(PPPL)
The eighteen excellent papers presented in this poster session covered a range
of topics relevant to plasma control and control systems.
Several papers focused on experience using feedback for plasma control and
equipment protection. D. Humphreys, et al., presented the "isoflux"
plasma shape multivariable control method as recently developed on the DIII-D
tokamak, based on simple linearized plasma response models and using feedback
from EFIT plasma edge shape/locations reconstructed from measurements every 1.5
milliseconds. M. Lennholm, et al., described an adaptive control system
used for the past year for automatic real-time tuning of JET's vertical
stabilization feedback loop. M.Matsukawa, et al., described experiences
from JT-60 poloidal field power supply modifications for high triangularity
divertor operation, including the successful simultaneous control of both
radial and vertical X-point location which was necessary to avoid tile damage,
and including the use of a rate limit to suppress oscillation in conjunction
with MHD instabilities and resulting overcurrent trips. S. Cox, et al.,
described the use of bremsstrahlung radiation measurements to prevent excessive
neutral beam shinethrough onto JET's torus walls, via a new interlock provided
for JET's active phase of tritium operations.
Several papers described how control systems were implemented in electronics
instrumentation and software. C. Takahashi, et al., described plasma
heating control and communication systems for the LHD experiment. R. Cool,
et al., described the control and protection systems for the TdeV
tokamak. M. Kawai, et al., described the computer control and data
acquisition system for JT-60U's negative ion neutral beam injector. P. Sichta,
et al., described the planned NSTX central instrumentation and control
system. T. Terakado, et al., described modernizing improvements of the
JT-60U control system to accommodate VME, networks, and UNIX workstations. D.
Ponce, et al., described the DIII-D tokamak's new ECH multiple control
system, implemented in software distributed over multiple computers interfaced
to a PLC, to a timing pulse system and to power supplies.
Several papers focused on computational methods to use in controls design and
analysis. J. Leuer, et al., presented probabilistic methods for
calculating likely stray fields on ITER, the ability to reduce them via
cancellation coils, and the likelihood of their creating locked modes in ITER's
plasma. R. Hatcher advanced an analytical formulation from electrical circuit
theory to use in stabilizing the "resistive wall mode" plasma instability. R.
Woolley presented methods to optimize design of nonaxisymmetric plasma feedback
systems. G. Chitarin, et al., presented methods for determining the
frequency-response transfer functions of the RFX device's shell and gap as
needed for local control of field errors, and compared calculation results to
experimental measurements.
Other papers addressed a range of subjects. H. Fernandes, et al.,
described special control details developed for continuous "ac" operation of
the ISTTOK tokamak. D. Desideri, et al., described design and
construction of a movable power electrode for the RFX device, to be used in
experiments attempting to improve confinement by modifying the ExB velocity
shear in the plasma edge region. H. Kugel, et al., discussed conceptual
designs for an experimental facility to evaluate active mode stabilization of
tokamak edge plasmas via biased electrodes and injected currents. V. Toigo,
et al., described the design of a possible system for the RFX device for
local field error reduction.
Altogether, papers presented this poster session formed a stimulating summary
of control issues important to fusion research in 1997.
P17: New and Proposed Machines, Mark Tillack (UCSD)
The ten posters in this session covered a range of new and innovative
confinement concepts, with some emphasis on plasma-based volumetric neutron
sources (VNS). Y. Ogawa described a superconducting tokamak VNS with R=4.5 m,
a=1 m, and driven by neutral beams to provide a neutron wall loading of the
order of 0.8 - 1.0 MW/m2. Using an enhanced, reversed-shear mode of
plasma operation, the wall loading could be extended to 1.4 MW/m2.
Tritium consumption is expected to be 10 kg/yr, necessitating a breeding
blanket; in this case, a PbLi breeder was employed. O. Filatov also described
a moderate aspect ratio (R=1.7, a=0.52 m) VNS, but using multi-turn "warm"
Cu-Cr-Zr alloy. The thrust of this paper was the detailed design and analysis
of the coil system, including the demountable joints.
Two papers treated the low aspect ratio "spherical tokamak" concept as a VNS.
The paper by E. T. Cheng overviewed the characteristics of an ST-VNS. The
device is designed to begin operation at a modest wall loading of 0.5
MW/m2, but is capable of running up to 5 MW/m2 following
validation of the in-vessel components. The ability of the device to fulfill
the testing needs for fusion technology development and demonstration was
highlighted with special consideration of the operating stages of the device.
The second paper by I. N. Sviatoslavsky focused on mechanical design
considerations for the ST-VNS. Thermal and structural analysis of the
centerpost were performed, and a maintenance scheme developed. The centerpost
in this design is single-turn, with a sliding joint at the top.
Four papers were presented on new confinement experiments: the HT-7U tokamak,
TJ-II stellarator, Globus-M spherical tokamak, and TODOROKI-1 force-balance
tokamak. HT-7U is a superconducting tokamak to be built at the Chinese Academy
of Sciences in Hefei. It will have long pulse capability (60-1000 s) with a
flexible PF coild system, several heating and current drive systems, and
ability to operate under various divertor and limter configurations. The TJ-II
stellarator is already assembled and nearly ready to operate in Spain. The
main experimental plan is to explore the effects of various magnetic field
configurations (with L=4), shear, toroidal current, etc. Globus-M is an A=1.5
ST to be constructed at the Ioffe institute in St. Petersburg. The design and
manufacture of the critical elements of the magnet systems were described. The
multi-turn central rod consists of 16 insulated bronze segments. Finally, a
force-balanced coil (FBC) has been been investigated both experimentally and as
a power plant candidate. FBC's use helical coils which carry both toroidal and
poloidal current. The goal is to cancel the centering force with the hoop
force in the FBC.
M. Irie presented a reactor concept using a moving ST core in a linear device.
Unlike the FRC, this device includes a stationary central conductor in the
forming region. An ST plasma is injected into the core of the device, at which
point it becomes a spheromak. Toroidal adiabatic compression plus MeV beams
are used to heat the plasma.
P18: Inertial Fusion Engineering, Jeff Latkowski (LLNL)
The six papers presented in this poster session addressed issues related to
laser fusion target production, experimental use of the National Ignition
Facility (NIF), progress in heavy-ion fusion (HIF) induction accelerators, and
the production of liquid-metal annular jets within reactor cavities. While most
of these papers focus on the near-term issues related to the operation of NIF,
others dealt with long-term issues of interest for inertial fusion energy
(IFE).
T. Norimatsu (ILE) presented the results of a new emulsion method that has been
used to produce polystyrene shells, some of which were close to NIF uniformity
goals. By using a rotating bed during drying, uniformity of > 98% was
achieved in 80% of the samples. R. B. Stephens (GA) discussed a technique of
producing target shells as thin as 1 mm and twice as large as those currently
shot on Nova. By allowing the shape to relax to a sphere prior to curing, they
have produced shells that have better surface roughness and are less
out-of-round than those currently available. N. B. Alexander (GA) presented
methods for in-situ, rapid assembly of NIF hohlraums. By delaying assembly of
the hohlraum until just before an experiment, D-T fill, layering, and
characterization may be simplified. Concepts that may be suitable for rapid
hohlraum assembly such as electrostatic, mechanical fastening, and laser
welding were analyzed.
P. F. Peterson and J. Scott (UCB) discussed issues related to the use of large
experimental packages in the NIF. For packages with minimal stand-off
distances from the target, x-ray ablation will generate conditions similar to
those envisioned for IFE target chambers. The authors make an argument for a
frost-coated mini-chamber for use in NIF operations.
M. Z. Hasan (Saga U.) presented an analytic method for the design of annular
liquid-lithium jets. Such jets may be used within an IFE target chamber to
protect the first wall and significantly increase its lifetime. The authors
used jet radius, thickness, velocity, inclination angle, and pressure drop as
parameters to control the cavity shape. Through use of as many as four jets,
nearly spherical cavities can be created.
A. Molvik (LLNL) presented results of performance studies for Metglas 2605SC
and 2605 SA1 for as magnetic cores in induction accelerating systems. Due to
the large masses of magnetic cores that would be required for a linac fusion
driver (> 107 kg), core performance and cost are critical issues. Results
for cores wound with mica paper and magnesium methylate insulators were
presented and alternatives such as parylene-N, kapton, and sodium salicylate
were discussed.
P19: Plasma Physics, Henry W. Kugel (PPPL)
A numerical simulation was used by Ohnishi, et al., to study the
evolution of the field-reversed configuration (FRC) by flux enhancement with a
rotating magnetic field. The plasma formed by a field reversed theta pinch was
evolved by numerically increasing the internal magnetic flux with an applied
rotating magnetic field (RMP) and by regulating the axial magnetic field. It
was found that the FRC plasma could be evolved and sustained if the energy
confinement time nearly satisfied the energy balance equilibrium during the
transition.
Preliminary studies of potential well measurements in Inertial-Electrostatic
Plasma Confinement Fusion (IECF) experiments were performed by Yamamoto, et
al. The IECF concept involves injecting ions and electrons through a
spherical grid towards the spherical center, trapping both species in the
resulting electrostatic self-field which givies rise to fusion reactions in the
dense core. In this work, a filament and an anode grid near the spherical
chamber wall were added to provide a double grid system. Measurements were
performed to compare the characteristics of double grid discharges with single
grid discharges. The neutron production rate of the double grid discharge was
about 25% larger than that of the single grid system. D-D neutron rates of
2x106/sec were obtained from 45 kV, 15 mA discharges.
The latest results of ITER fusion performance projections and operation
modeling were presented by Boucher et al. A set of "physics rules"
summarizing the present knowledge of plasma physics and tokamak operation
relevant to ITER have been developed and implemented in at least five transport
codes presently in use (PRETOR, ASTRA, BALDUR, TRANSP, GTWHIST). These codes
have been used to evolve the plasma equilibrium, temperature, and density as a
function of time and radius. The simulations indicate that even under
conditions of very poor confinement (HH=0.55), the goal of 1500 MW of fusion
power can be achieved by raising the auxiliary power to 150 MW and the plasma
current to 24 MA, and operating at densities exceeding the Greenwald limit.
Numerical studies also have demonstrated that simultaneous control can be
achieved over the fusion power output, the divertor input power, and the main
operating conditions by active feedback control of the auxiliary heating, the
D-T gas injection rate, and the high Z impurity seeding.
The results of a theoretical study of prospects for Electron Cyclotron Current
Drive (ECCD) stabilization of neoclassical tearing modes in ITER were presented
by Perkins, et al. Neoclassical islands are observed to arise at the
major rational surfaces of many tokamaks and can degrade confinement and
performance (b-limits, disruptions, etc.).
Recent work implies that they
may arise due to the loss of bootstrap current density. The results indicate
that temporal modulation will suffice for rotating modes; ECCD stabilization
of locked modes will require 4 ECCD launcher ports spaced toroidally.
Preliminary ray-tracing results indicate that a 50 MW ECCD system for ITER can
fulfill the derived stabilization criteria and provide bootstrap current levels
of 0.1 MA/m2.
Meade presented an analysis which noted that fusion power Q, break-even, and
the ntE diagram are well defined and
understood for steady state
plasma conditions but that it was necessary to clarify the definitions for
transient plasmas. In the earlier definition, which was used by TFTR,
break-even (Pfusion = Paux) occurs at Q =1, ignition
occurs at Q = infinity and ntE*
values required to achieve a
given Q are the same in transient and steady-state plasmas. The more recent
JET/JT-60 methods use definitions which include the input power required to
change the internal plasma energy, dWp/dt, in the definitions of Q
and tE. This method produces the
confusing result that
break-even requires Q* = Paux / (Paux -
dWp/dt) which is >1 for many cases of interest. In addition, the
ntE value required to achieve break-even
depends on
dWp/dt and therefore experimental data points with different
dWp/dt must be compared to different Q* curves on the Lawson
diagram. For a pulsed plasma, this issue can be avoided by using the original
Lawson definition Q = fusion energy per pulse divided by the auxiliary plasma
heating energy supplied per pulse.
The effect of atomic and molecular elastic collisions in the edge region and
divertor of ITER was discussed by Ruzic and Hayden. The detailed neutral gas
behavior of the ITER reference geometry was studied with the newly enhanced
DEGAS+ computer code. These ion-neutral collisions are particularly important
in two regions: (1) the puffing of neutral molecules from gas valves located
near the top of the machine, and (2) the low temperature plasma near the walls
which recycles a significant number of molecules due to low energy ions
recombining at the saturated surface, being released, and subsequently,
scattered back to the wall to enhance chemical sputtering. The results of the
simulations indicate that inclusion of elastic scattering is critical for
calculating proper flux and energy distributions, and that chemical sputtering
by non-thermal molecules must be assessed. In the case of gas puffing, it was
found that realistic geometry must be included when simulating gas-puffing, and
gas puffing must be diffuse and distributed to prevent unacceptable erosion
from charge exchange.
An edge plasma analysis for the KSTAR divertor design using the UEDGE, B2.5,
and DEGAS computer codes was presented by Im, et al. The UEDGE 2-D
multi-fluid edge plasma transport code was used to determine heat and particle
fluxes and plasma temperatures at the 45 deg. tilted divertor plate
with pumping effects. The B2.5 code was used to find suitable KSTAR divertor
leg length by varying the divertor channel width and depth along with the
variation of temperature and density of core plasmas. The DEGAS Monte-Carlo
neutral transport code was used to study core fueling of recycled neutrals for
various baffle configurations including variation of gap distance and baffle
shapes. Work is in progress to optimize the divertor region geometry and
pumping to minimize core fueling.
Zwicker et al., discussed using the INTERNET for plasma physics
education. The current reform in K-12 science education is based on current
research examining the best practice in science learning and teaching, which
has resulted in the creation of curricula that are student-led, hands-on, and
open-ended. The INTERNET adds a unique dimension to the possible ways
computers can be used as a learning tool. The Internet Plasma Physics
Experience (IPPEX) was created and modeled upon these principles to teach
middle and high school students about plasma physics and fusion energy.
Sections in IPPEX module include a virtual tokamak, analysis of data from the
TFTR experiment, and "ask a scientist". Over 11,000 people have visited the
site in the last 8 months.
P20: Blanket, Shield and Vacuum Vessel Engineering, Dai Kai Sze
(ANL)
This session had 11 papers. The first paper discussed the design of the helium
loops for the ITER Helium Cooled Pebble Bed (HCPB) test blanket module. Three
helium loops are required for: (a) tritium extraction, (b) heat removal, and
(c) coolant purification. The main design data as well as flow diagrams of the
loops are presented. Verification of the design and testing for reliable
operation with respect of process control and chemical analysis will be
required.
There were two papers for the ITER blanket design. The first one is titled
"Progress in the ITER Blanket Design" described the design of the shielding
blanket for the ITER BPP. Significant improvement of the ITER blanket were
possible with the better definition of the thermal and electromagnetic effects.
A supporting double wall backplate with reinforcement about the ports are
defined. The second one is entitled "The European Breeding Blanket Design for
ITER". This paper described the design of the breeding blanket for the ITER
EPP. The main features of this design are (a) the use of beryllium in the form
of pebble bed, (b) the adoption of flat radial-poloidal cooling pennels, and
(c) the confinement of the breeder pebbles in poloidal oriented circular
elements. A globe tritium breeding ratio of 1.01 for full coverage is
reported.
Another paper entitled "Lifetime Estimation of a Possible ITER EPP Blanket" was
presented. The paper estimates the life time of the ITER first wall, use the
first wall configuration and coolant flow parameters of the He-cooled,
martensitic steel, European blanket design proposed for the DEMO, and assuming
loading conditions anticipated in the ITER EPP. The calculations and analysis
of the results suggest that the zero-fatigue lifetime (creep damage only) for
the low coolant temperature (315.5 C) is 6.2 years, and for high coolant
temperature (375 C is 3.08 years.
There were two papers on the ITER shielding design. The paper entitled "Profit
from Borating Concrete in the ITER Biological Shield" concluded that, by adding
0.1 g/cm3 of boron in the concrete, the does rate can be reduced by
a factor of 2-3 behind the biological shield. The paper entitled "Status of
the Radiation Shielding Analysis for ITER" used Monte Carlo calculations to
estimate the shielding requirements for the ITER divertor pumping and remote
handling ports and the impact on the cryostat does rate of neutron streaming
through a poorly shielded equatorial port. Properly design shield can assure
personnel access (< 200 uSv/h) at ~ 10 days after reactor shutdown.
One paper proposed an advanced blanket design (High-Performance PbLi Blanket).
The proposed design is a dual coolant concept based on ferritic steel as the
structural material being cooled by He. The breeding material is LiPb which is
also used as coolant to remove the nuclear heating. A SiC layer is used both
as a flow channel inserts to reduve the MHD pressure drop of the LiPb, and also
acts as thermal insulator to separate the LiPb temperature from the steel
temperature. A LiPb exit temperature of 700C can be obtained. A (He+LiPb) to
He heat exchanger transfers the thermal energy to a secondary He stream, which
will operate a closed-cycle helium gas turbine, with an estimated gross thermal
efficiency of 45%.
There were four papers on the vacuum vessel designs for ITER, KSTAR and SSTI.
They provided the design description and design analysis of the vacuum
vessels.
P21: Power Plant Studies, R. L. Miller (UCSD)
Seven posters were presented in this session. The majority of the
presentations dealt with magnetic fusion energy (MFE), specifically tokamak,
approaches.
Three presentations discussed aspects of the U.S. ARIES Team conceptual design
study of a Spherical Tokamak (ST) 1,000-MWe class central power station. T.-K.
Mau (UCSD) et al. summarized the plasma physis basis of the
low-aspect-ratio ST, empahasizing high beta and high bootstrap currents
relative to conventional tokamaks. Properties of the MHD equilibrium for
aspect ratios in the range 1.4-1.8, as well as issues of profile control and
plasma start-up were included. W. Reiersen (PPPL) et al. considered
centerpost (i.e., inboard toroidal field coil) design options for the
ST, taking into account configurations and materials choices appropriate for
resistive magnetic coils. X. R. Wang (UCSD) et al. considered overall
configuration and maintenance options for the ST, aiming to maximize
operational availability and thus incur savings in the projected cost of
electricity (COE). An alternative and more optimistic characterization of the
ST power plant was presented by C. P. C. Wong (GA) et al.
Another power plant projection, denoted CREST-1 (Compact REversed Shear
Tokamak) was described by K. Okano (CRIEPI) et al. It emphasized
operational flexibility for partial load operation by combined neutral beam and
rf current drive and profile control. The RS approach represents an important
avenue for tokamak concept improvement.
Turning to inertial fusion energy (IFE), R. W. Moir (LLNL) outlined the
interaction of available and projected options (targets, illuminators,
chambers, and optics protection) as key considerations in the advancement of
IFE along a development path pointing to an economically competitive power
plant.
L. M. Waganer (Boeing) presented a methodology and sample results for
evaluating possible non-electric applications of fusion that might be expected
to broaden the market base or accelerate the practical introduction of fusion
devices by exploiting the neutron or radiation products. Promising applications
include transmutation of nuclear (fission) wastes, hydrogen production,
radio-isotope production, and future space propulsion.
O1: Tokamak Engineering and Operations, Osamu Motojima (NIFS)
Oral Sessions
Poster Sessions