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IEEE Transactions on Applied Superconductivity | 2008

The ITER Magnet System

N. Mitchell; D. Bessette; R. Gallix; C. Jong; J. Knaster; P. Libeyre; C. Sborchia; F. Simon

Procurement of the ITER magnets is due to start at the end of 2007/early 2008, with the launch of the longest lead time items, the conductor and the TF coil windings. The base design for procurement was established in 2001, and the build up of the Cadarache ITER team has been accompanied by a review of the most critical, or controversial, features of the 2001 design. At the same time, an urgent R&D program has been launched to complete the necessary verification of the design solutions that are proposed. In this paper an overview will be presented of the main design features and drivers, and some of the recent issues and R&D results will be summarized.


IEEE Transactions on Applied Superconductivity | 2012

Status of ITER Conductor Development and Production

Arnaud Devred; Ina Backbier; D. Bessette; Gregory Bevillard; Mark Gardner; Mathew Jewell; N. Mitchell; Ian Pong; Alexander Vostner

The ITER magnet coils are wound from Cable-In-Conduit Conductors (CICC) made up of superconducting and copper strands assembled into a multistage, rope-type cable inserted into a conduit of butt-welded austenitic steel tubes. The conductors for the Toroidal Field (TF) and Central Solenoid (CS) coils require about 500 tons of Nb3Sn strands while the Poloidal Field (PF) and Correction Coil (CC) conductors need around 250 tons of Nb-Ti strands. The required amount of Nb3Sn strands far exceeds pre-existing industrial capacity and calls for a significant worldwide production scale up. After explaining the in-kind procurement sharing of the various conductor types among the six ITER Domestic Agencies (DA) involved: China, Europe, Japan, South Korea, Russia, and the United States, we detail the technical requirements defined by the ITER International Fusion Energy Organization (IO), and we present a brief status of ongoing productions. The most advanced production is that for the TF conductors, where all six DAs have qualified suppliers and about 50% of the required strands have been produced and registered into the web-based conductor database developed by the IO.


Superconductor Science and Technology | 2014

Challenges and status of ITER conductor production

Arnaud Devred; I Backbier; D. Bessette; Gregory Bevillard; M Gardner; C Jong; F Lillaz; N. Mitchell; Gennaro Romano; Alexander Vostner

Taking the relay of the large Hadron collider (LHC) at CERN, ITER has become the largest project in applied superconductivity. In addition to its technical complexity, ITER is also a management challenge as it relies on an unprecedented collaboration of seven partners, representing more than half of the world population, who provide 90% of the components as in-kind contributions. The ITER magnet system is one of the most sophisticated superconducting magnet systems ever designed, with an enormous stored energy of 51?GJ. It involves six of the ITER partners. The coils are wound from cable-in-conduit conductors (CICCs) made up of superconducting and copper strands assembled into a multistage cable, inserted into a conduit of butt-welded austenitic steel tubes. The conductors for the toroidal field (TF) and central solenoid (CS) coils require about 600?t of Nb3Sn strands while the poloidal field (PF) and correction coil (CC) and busbar conductors need around 275?t of Nb?Ti strands. The required amount of Nb3Sn strands far exceeds pre-existing industrial capacity and has called for a significant worldwide production scale up. The TF conductors are the first ITER components to be mass produced and are more than 50% complete. During its life time, the CS coil will have to sustain several tens of thousands of electromagnetic (EM) cycles to high current and field conditions, way beyond anything a large Nb3Sn coil has ever experienced. Following a comprehensive R&D program, a technical solution has been found for the CS conductor, which ensures stable performance versus EM and thermal cycling. Productions of PF, CC and busbar conductors are also underway. After an introduction to the ITER project and magnet system, we describe the ITER conductor procurements and the quality assurance/quality control programs that have been implemented to ensure production uniformity across numerous suppliers. Then, we provide examples of technical challenges that have been encountered and we present the status of ITER conductor production worldwide.


IEEE Transactions on Applied Superconductivity | 2002

Test of the ITER central solenoid model coil and CS insert

N. Martovetsky; P.C. Michael; J.V. Minervini; A. Radovinsky; Makoto Takayasu; C. Gung; R. Thome; T. Ando; Takaaki Isono; Kazuya Hamada; Takashi Kato; Katsumi Kawano; Norikiyo Koizumi; K. Matsui; Hideo Nakajima; Gen Nishijima; Y. Nunoya; M. Sugimoto; Y. Takahashi; H. Tsuji; D. Bessette; K. Okuno; N. Mitchell; M. Ricci; Roberto Zanino; Laura Savoldi; K. Arai; Akira Ninomiya

The Central Solenoid Model Coil (CSMC) was designed and built from 1993 to 1999 by an ITER collaboration between the U.S. and Japan, with contributions from the European Union and the Russian Federation. The main goal of the project was to establish the superconducting magnet technology necessary for a large-scale fusion experimental reactor. Three heavily instrumented insert coils were built to cover a wide operational space for testing. The CS Insert, built by Japan, was tested in April-August of 2000. The TF Insert, built by Russian Federation, will be tested in the fall of 2001. The NbAl Insert, built by Japan, will be tested in 2002. The testing takes place in the CSMC Test Facility at the Japan Atomic Energy Research Institute, Naka, Japan. The CSMC was charged successfully without training to its design current of 46 kA to produce 13 T in the magnet bore. The stored energy at 46 kA was 640 MJ. This paper presents the main results of the CSMC and the CS Insert testing-magnet critical parameters, ac losses, joint performance, quench characteristics and some results of the post-test analysis.


Nuclear Fusion | 2001

Progress of the ITER central solenoid model coil programme

Hiroshi Tsuji; K. Okuno; R. Thome; E. Salpietro; S. Egorov; N. Martovetsky; M. Ricci; Roberto Zanino; G. Zahn; A. Martinez; G. Vecsey; K. Arai; T. Ishigooka; T. Kato; Toshinari Ando; Yoshikazu Takahashi; H. Nakajima; T. Hiyama; M. Sugimoto; N. Hosogane; M. Matsukawa; Y. Miura; T. Terakado; J. Okano; K. Shimada; M. Yamashita; Takaaki Isono; Norikiyo Koizumi; Katsumi Kawano; M. Oshikiri

The worlds largest pulsed superconducting coil was successfully tested by charging up to 13 T and 46 kA with a stored energy of 640 MJ. The ITER central solenoid (CS) model coil and CS insert coil were developed and fabricated through an international collaboration, and their cooldown and charging tests were successfully carried out by international test and operation teams. In pulsed charging tests, where the original goal was 0.4 T/s up to 13 T, the CS model coil and the CS insert coil achieved ramp rates to 13 T of 0.6 T/s and 1.2 T/s, respectively. In addition, the CS insert coil was charged and discharged 10 003 times in the 13 T background field of the CS model coil and no degradation of the operational temperature margin directly coming from this cyclic operation was observed. These test results fulfilled all the goals of CS model coil development by confirming the validity of the engineering design and demonstrating that the ITER coils can now be constructed with confidence.


IEEE Transactions on Applied Superconductivity | 2005

Test results of the ITER PF insert conductor short sample in SULTAN

Pierluigi Bruzzone; M. Bagnasco; D. Bessette; D. Ciazynski; A. Formisano; P. Gislon; F. Hurd; Y. Ilyin; R. Martone; N. Martovetsky; L. Muzzi; Arend Nijhuis; H. Rajainmaki; C. Sborchia; Boris Stepanov; L. Verdini; Rainer Wesche; L. Zani; Roberto Zanino; E. Zapretilina

A short sample of the NbTi cable-in-conduit conductor (CICC) manufactured for the ITER PF insert coil has been tested in the SULTAN facility at CRPP. The short sample consists of two paired conductor sections, identical except for the sub-cable and outer wraps, which have been removed from one of the sections before jacketing. The test program for conductor and joint includes DC performance, cyclic load and AC loss, with a large number of voltage taps and Hall sensors for current distribution. At high operating current, the DC behavior is well below expectations, with temperature margin lower than specified in the ITER design criteria. The conductor without wraps has higher tolerance to current unbalance. The joint resistance is by far higher than targeted.


Superconductor Science and Technology | 2012

Results of the TF conductor performance qualification samples for the ITER project

Marco Breschi; Arnaud Devred; Marco Casali; D. Bessette; M. C. Jewell; N. Mitchell; I. Pong; A. Vostner; Pierluigi Bruzzone; Boris Stepanov; Thierry Boutboul; N. Martovetsky; Keeman Kim; Y. Takahashi; V Tronza; Wu Yu

The performance of the toroidal field (TF) magnet conductors for the ITER machine are qualified by a short full-size sample (4 m) current sharing temperature (T-cs) test in the SULTAN facility at CRPP in Villigen, Switzerland, using the operating current of 68 kA and the design peak field of 11.8 T. Several samples, including at least one from each of the six ITER Domestic Agencies participating in TF conductor fabrication (China, European Union, Japan, Russia, South Korea and the United States), have been qualified by the ITER Organization after achieving T-cs values of 6.0-6.9 K, after 700-1000 electromagnetic cycles. These T-cs values exceed the ITER specification and enabled the industrial production of these long-lead items for the ITER tokamak to begin in each Domestic Agency. Some of these samples did not pass the qualification test. In this paper, we summarize the performance of the qualified samples, analyze the effect of strand performance on conductor performance, and discuss the details of the test results.


IEEE Transactions on Applied Superconductivity | 2013

Status of Conductor Qualification for the ITER Central Solenoid

Arnaud Devred; D. Bessette; Pierluigi Bruzzone; K. Hamada; Takaaki Isono; N. Martovetsky; N. Mitchell; Y. Nunoya; K. Okuno; I. Pong; W. Reiersen; C. M. Rey; Boris Stepanov; Y. Takahashi; A. Vostner

The ITER central solenoid (CS) must be capable of driving inductively 30 000 15 MA plasma pulses with a burn duration of 400 s. This implies that during the lifetime of the machine, the CS, comprised of six independently powered coil modules, will have to sustain severe and repeated electromagnetic cycles to high current and field conditions. The design of the CS calls for the use of cable-in-conduit conductors made up of and pure copper strands, assembled in a five-stage, rope-type cable around a central cooling spiral that is inserted into a circle-in-square jacket made up of a special grade of high manganese stainless steel. Since cable-in-conduit conductors are known to exhibit electromagnetic cycling degradation, prior to the launch of production, the conductor design and potential suppliers must be qualified through the successful testing of full-size conductor samples. These tests are carried out at the SULTAN test facility. In this paper, we report the results of the on-going CS conductor performance qualification and we present the options under consideration for the different modules constituting the CS coil.


IEEE Transactions on Applied Superconductivity | 2010

Overview of the ITER Correction Coils Design

A. Foussat; P. Libeyre; N. Mitchell; Y. Gribov; C. Jong; D. Bessette; R. Gallix; Pierre Bauer; A. Sahu

The Correction Coils (CC) of the ITER Tokamak are developed to reduce the range of magnetic error fields created by imperfections in the location and geometry of the other coils used to confine, heat, and shape the plasma. The proposed system consists of three sets of 6 coils each, located at the top (TCC), side (SCC) and bottom (BCC) of the Tokamak device and using a NbTi cable-in-conduit superconducting conductor (CICC). Within each set, the coils are connected in pairs to produce a toroidal field to reduce the most troublesome, lower order, poloidal mode number fields (m = 1,2,3) in order to operate below the locked mode threshold. The conductor is designed to operate up to 6 T. The winding uses pancakes of one-in-hand conductor (quadpancakes for SCC, octopancakes for TCC and BCC), thus avoiding internal joints. The winding-pack is enclosed inside a 20 mm thick stainless steel casing. The coils are supported by rigid connections to the Toroidal Field (TF) coils. The structural design of the CC is mainly driven by the allowable fatigue stress levels in the conductor jacket, in the case material and in the glass-polyimide electrical insulation system. The boundary conditions on the CC are imposed by the TF coils deformation and the electromagnetic interactions with the PF coils system. The thermo-hydraulic and electrical performance of the CICC is also addressed.


IEEE Transactions on Applied Superconductivity | 2009

Test Results From the PF Conductor Insert Coil and Implications for the ITER PF System

D. Bessette; L. Bottura; Arnaud Devred; N. Mitchell; K. Okuno; Y. Nunoya; C. Sborchia; Y. Takahashi; Arjan Verweij; A. Vostner; Roberto Zanino; E. Zapretilina

In this paper we report the main test results obtained on the Poloidal Field Conductor Insert coil (PFI) for the International Thermonuclear Experimental Reactor (ITER), built jointly by the EU and RF ITER parties, recently installed and tested in the CS Model Coil facility, at JAEA-Naka. During the test we (a) verified the DC and AC operating margin of the NbTi Cable-in-Conduit Conductor in conditions representative of the operation of the ITER PF coils, (b) measured the intermediate conductor joint resistance, margin and loss, and (c) measured the AC loss of the conductor and its changes once subjected to a significant number of Lorentz force cycles. We compare the results obtained to expectations from strand and cable characterization, which were studied extensively earlier. We finally discuss the implications for the ITER PF system.

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N. Martovetsky

Oak Ridge National Laboratory

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Takaaki Isono

Japan Atomic Energy Agency

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Pierluigi Bruzzone

École Polytechnique Fédérale de Lausanne

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Boris Stepanov

École Polytechnique Fédérale de Lausanne

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