17th IEEE/NPSS Symposium on Fusion Engineering

Summary of the 17th IEEE/NPSS Symposium on Fusion Engineering, San Diego, California,

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 Sessions

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.


Oral Sessions

O1: Tokamak Engineering and Operations, Osamu Motojima (NIFS)

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.


Poster Sessions

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.

P22: Neutral Beam Injection and Fueling Systems, Alfred von Halle (PPPL)

This poster session presented papers that discussed recent developments and results in the areas of neutral beams and fueling systems. There were eleven posters covering a nice mix of material on operating and recently operated systems, new designs for future machines, and reports on new technological developments of general interest.

In there area of new technologies, Thomcast, a division of Thomson-CSF, presented a design for a high voltage power supply based on the Pulse Step Modulator (PSM) technology developed by Brown Boveri (BBC). Oak Ridge National Laboratories (ORNL) reported on work in progress on curved guide tubes for pellet injectors. ORNL is presently testing curved guide pellet injection systems for 2.7-mm pellets (DIII-D relevant) and 10-mm pellets (ITER relevant).

Recent design elements of neutral beam systems for ITER and SST-1 were presented. The Japanese Atomic Energy Research Institute (JAERI) reported on recent progress on the development of the high power negative ion source/accelerator for the ITER-NBI. The JAERI negative ion beam system has produced a stable hydrogen beam for 1 second at 868 keV and 19 mA using a five stage electrostatic accelerator. It has also produced a deuterium beam at 380 kev, 14.3 A and a hydrogen beam at 350 keV, 18.4 A. The SST-1 group presented a proposed design of a compact beam line for the SST-1 NBI which considered beam transmission, pressure profiles, reionization losses and duct transmission losses for a beamline based on a duct size of 19 cm by 35 cm and anticipated heat loads of 1kW/cm2. The SST-1 also presented, in a seperate paper, a design for an ion deflection system capable of deflecting and dissipating 2.5 MW at 80 keV within the the maximum specified power density of 1kW/cm2 on ion dump surfaces.

Recent results of neutral beam injection and fueling systems operating on DIII-D, JET, JT-60, and TFTR were presented. There were three posters reporting on data taken during the final operating campaign of the TFTR neutral beam systems. These provided information on the tritium consumption and retention in the TFTR beamlines, analyses of TFTR ion source grid and arc chamber failures sustained during high power operations in deuterium and tritium, and engineering studies of the maximum pulse length obtainable using the U.S. Common Long Pulse Ion Source on a TFTR beamline. The JET group reported on their highly successful tritium neutral beam operations using an active-phase gas introduction system in achieving 160 keV beam energies. DIII-D reported on a recently completed study comparing the calculated shine through of the neutral beams in the DIII-D plasma to measured values inferred from the target temperature rises, finding good agreement extrapolated over a range of power densities. JT-60 reported on the ongoing progress of the high voltage power supply used to support their negative ion based neutral beam injection system.

P23: Power Systems, Pier Luigi Mondino (ITER-Naka)

TdeV Power Supplies Interaction with the Utility Power Grid (D. Larose). The tokamak TdeV was recently up-graded: new power supplies were added to the existing ones. The total installed power is now 110 MVA. The HV Grid, to which the TdeV is connected, could not cope with the new loads: reactive power compensation and harmonic filtering were required. This is achieved with 14 capacitor banks, switched on and off in sequence, with vacuum switches. To avoid voltage transients the switching is fully syncronized with the phase voltage zero. The experimental results compare well with computer simulations both on voltage drops and on harmonics. (Note: reactive power compensation and harmonic filtering, with the same approach, were added at JET, several years ago and the results were reported at the SOFT, Roma, 1992).

Windage Loss Reduction Study for TFTR-Pulse Generator (M. N. Awad). This paper reported the results of a detailed study aimed to reduce the ventilation losses on TFTR MG sets. It was found that the air velocity could be reduced maintaining the conductor temperatures within limits acceptable for the insulation. The modification allows a power saving of 200 kW; the related cost saving also was evaluated.

The Development and Testing of a 66kA By-Pass Switch with ARC Commutation Capability for the ITER Coil Power Supply System (T. Bonicelli). This paper described firstly the modifications done to an existing industrial switch to allow it to satisfay the ITER requirements and secondly it reports the results of the extensive tests performed so far. Among others, the commutation of the current from the by-pass switch to the parallel vacuum circuit breaker was investigated in detail, the results are very encouraging: the commutation time is about 5 ms. Finally the paper reported also the modifications identified after the tests to improve further the switch performance. This paper shows an excellent example of fruitful cooperation among ITER JCT staff, Home Team staff from laboratories and from industries on the development of an essential component -- the "by-pass switch" -- far beyond its original industrial capabilities.

Power Supply System for 1000 s Neutral Beam Injector (U. K. Baruah). This paper described the design of the power system for the 80-kV, 100-A neutral beam for the SST-1 tokamak. The acceleration power supply foresees the use of Pulse Step Modulator (PSM), a system developed by an European industry for short wave and medium wave power transmitters. The PSM has already been used for the NB power supply in Textor. The paper also described the design of the auxiliary power supplies, of the transmission line and of the snubber circuit. The technical details, reported in the paper, give confidence on the soundness of this design of the neutral beam power supply.

Design, Construction and Operation of the 66 kA Life Test Facility for ITER Magnet Protection Vacuum Circuit Breakers (P. Campostrini and A. Maschio). This paper described the test facility built at the Consorzio RFX, Padova Italy, to perform life tests on a vacuum circuit breaker developed starting from an industrial component. The paper described firstly the dummy load and the connecting lines, the AC/DC converters, the counter-pulse network, the measurement and protection system and finally the control and data acquisition. In the second part the test results were presented: about 1600 interruptions were performed (with 7 restrikes). This paper shows an excellent example of fruitful cooperation among ITER Home Team staff from laboratories and from industries on the development of an essential component -- "the vacuum circuit breaker" -- far beyond its original industrial capabilities.

Bypass Operation of the ITER ac/dc Converters for Reactive Power Reduction (E. Gaio and R. Piovan). The first part of this paper reviewed an interesting approach to reactive power compensation, previously presented in other papers. Then the internal bypass operation was discussed: the transition from normal operation to the bypass mode and vice versa can be performed, avoiding current imbalance, only under well identified conditions. Moreover, the current imbalance under fast output voltage variation was investigated. The theoretical analysis, done on a simplified model, and the computer simulations, done with a realistic model of the converter, allow identification of the minimum delays required for the transitions. This paper shows another case of fruitful cooperation among ITER JCT staff and Home Team staff from laboratories on an interesting design issue -- "bypass operation of ac/dc converters" -- for protection and for reactive power reduction.