Mini-RT. Plasma Production and Levitation Experiments of a High-temperature Superconductor Coil in a Mini-RT Internal Coil Device

Similar documents
Defense Technical Information Center Compilation Part Notice

Magnetic Field Configuration Dependence of Plasma Production and Parallel Transport in a Linear Plasma Device NUMBER )

Formation of High-b ECH Plasma and Inward Particle Diffusion in RT-1

Innovative fabrication method of superconducting magnets using high T c superconductors with joints

Feasibility of HTS Magnet Option for Fusion Reactors )

DT Fusion Ignition of LHD-Type Helical Reactor by Joule Heating Associated with Magnetic Axis Shift )

Reconstruction of Pressure Profile Evolution during Levitated Dipole Experiments

Stabilization of a low-frequency instability inadipoleplasma

Pulse field magnetization of a ring-shaped bulk superconductor

Reconstruction of the Pressure Profile of LDX High Beta Plasma

Dynamics of Drift and Flute Modes in Linear Cylindrical ECR Plasma

MHD instability driven by supra-thermal electrons in TJ-II stellarator

Experiments with a Supported Dipole

Electromagnetic Design of 10 MW Class Fully Superconducting Wind Turbine Generator

Manufacturing of LTS and HTS Magnets for Heavy- Ion Rotating Gantry

Role of the Electron Temperature in the Current Decay during Disruption in JT-60U )

Superconducting Magnet Design and R&D with HTS Option for the Helical DEMO Reactor

Status of A Positron-Electron Experiment (APEX) towards the formation of pair plasmas

High Beta Discharges with Hydrogen Storage Electrode Biasing in the Tohoku University Heliac

The Effect of Cooling Systems on HTS Microstrip Antennas

Bi Current Sharing among Filaments for Bi-2223 Ag-sheathed Tapes with Inter-filament Barrier

Critical Current Properties of HTS Twisted Stacked-Tape Cable in Subcooled- and Pressurized-Liquid Nitrogen

Physics and Operations Plan for LDX

Intermittent Behavior of Local Electron Temperature in a Linear ECR Plasma )

Confinement of toroidal non-neutral plasma in Proto-RT

Confinement of toroidal non-neutral plasma in Proto-RT

What we ve learned so far about the Stability of Plasma Confined by a Laboratory Dipole Magnet

Design of a laminated-steel magnetic core for use in a HT-SMES

Reduced-Size LHD-Type Fusion Reactor with D-Shaped Magnetic Surface )

Development of Remountable Joints and Heat Removable Techniques for High-temperature Superconducting Magnets

Density Collapse in Improved Confinement Mode on Tohoku University Heliac

Magnetic Diagnostics Basics

The Effects of Noise and Time Delay on RWM Feedback System Performance

Flux Motion and Screening Current in High-temperature Superconducting Magnets

Magnetic Field Design for a 2.45-GHz ECR Ion Source with Permanent Magnets

Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:

Double Null Merging Start-up Experiments in the University of Tokyo Spherical Tokamak

Effect of Biasing on Electron Temperature in IR-T1 Tokamak

Prospects for Driven Particle Convection Tests in LDX. Abstract

Kalman Filter for Noise Reduction and Dynamical Tracking for Levitation Control and for Plasma Mode Control

The Status of the Design and Construction of the Columbia Non-neutral Torus


SIMULATIONS OF ECR PROCESSING SYSTEMS SUSTAINED BY AZIMUTHAL MICROWAVE TE(0,n) MODES*

Spatial and Temporal Variations of a Screening Current Induced Magnetic Field in a Double-Pancake HTS Insert of an LTS/HTS NMR Magnet

Magnetic Levitation without Feedback Control

Title use of Bi-2223/Ag squirrel-cage rot IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY (2006), 16(2): 14.

Development of a dispersion interferometer for magnetic confinement plasma and its application to atmospheric pressure plasmas

Confinement of toroidal non-neutral plasma

HTS Magnets for Accelerator Applications

Generation and Characterization of High Heat-Flux Plasma-Flow for Divertor Simulation Studies Using a Large Tandem Mirror Device

Experimental Investigation of High-Temperature Superconducting Magnet for Maglev

Physica C 468 (2008) Contents lists available at ScienceDirect. Physica C. journal homepage:

Behavior of Compact Toroid Injected into the External Magnetic Field

Inductance and Current Distribution Analysis of a Prototype HTS Cable

The compact dipole configuration for plasma confinement

Helium Catalyzed D-D Fusion in a Levitated Dipole

ECR ION SOURCES : A BRIEF HISTORY AND LOOK INTO THE NEXT GENERATION

Fluctuation Suppression during the ECH Induced Potential Formation in the Tandem Mirror GAMMA 10

Analytical Study of RWM Feedback Stabilisation with Application to ITER

Electrostatic Interchange Instabilities of a Rotating, High-Temperature Plasma Confined by a Dipole Magnet: Experiment and Theory

Impact of High-Temperature Superconductors on the Superconducting Maglev

Overview and Experimental Program of the Levitated Dipole Experiment

DEVELOPMENT AND PRODUCTION OF SUPERCONDUCTING AND CRYOGENIC EQUIPMENT AND SYSTEMS FOR ACCELERATORS BY IHEP

On Dust Particle Dynamics in Tokamak Edge Plasma

CBSE Sample Paper 7. Question 1 What is the ratio of radii of the orbits corresponding to first excited state and ground state in a hydrogen atom?

Implementation of a long leg X-point target divertor in the ARC fusion pilot plant

Ch. 3. Pulsed and Water Cooled Magnets. T. J. Dolan. Magnetic field calculations

Effects of Noise in Time Dependent RWM Feedback Simulations

Accelerators. Table Quadrupole magnet

Material, Design, and Cost Modeling for High Performance Coils. L. Bromberg, P. Titus MIT Plasma Science and Fusion Center ARIES meeting

Design of structural components and radial-build for FFHR-d1

Measurement of the Density Profile of a Toroidal Non-neutral Plasma with a Wall-Probe Array

NONLINEAR CONTROL OF A MAGNETIC LEVITATION SYSTEM USING FEEDBACK LINEARIZATION

Physics and Engineering Studies of the Advanced Divertor for a Fusion Reactor

Axial Magnetic Field of Superconducting Loops

1 EX/C4-3. Increased Understanding of Neoclassical Internal Transport Barrier on CHS

High-Performance Y-based Superconducting Wire and Their Applications

Title. Author(s)Terauchi, N.; Noguchi, S.; Igarashi, H. CitationPhysica C: Superconductivity, 471(21-22): Issue Date Doc URL.

Keywords: Superconducting Fault Current Limiter (SFCL), Resistive Type SFCL, MATLAB/SIMULINK. Introductions A rapid growth in the power generation

Production of Over-dense Plasmas by Launching. 2.45GHz Electron Cyclotron Waves in a Helical Device

Nano-ECRIS project: a new ECR ion source at Toyo University to produce endohedral fullerenes

Small Spherical Tokamaks and their potential role in development of fusion power

Comparison of Trapped Field Characteristic of Bulk Magnet System Using Various Type Refrigerators

Strong High-Temperature Superconductor Trapped Field Magnets

Generation and Acceleration of High-Density Helicon Plasma Using Permanent Magnets for the Completely Electrodeless Propulsion System )

INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL

MODELING OF AN ECR SOURCE FOR MATERIALS PROCESSING USING A TWO DIMENSIONAL HYBRID PLASMA EQUIPMENT MODEL. Ron L. Kinder and Mark J.

Simulation Study of High-Frequency Magnetosonic Waves Excited by Energetic Ions in Association with Ion Cyclotron Emission )

Noninductive Formation of Spherical Tokamak at 7 Times the Plasma Cutoff Density by Electron Bernstein Wave Heating and Current Drive on LATE

Evaluation of Quasi-Steady Operation of Applied Field 2D- MPD Thruster using Electric Double-Layer Capacitors

Recent results on non-inductive startup of highly overdense ST plasma by electron Bernstein wave on LATE

Design and Experimental Evaluation of the Flywheel Energy Storage System

The Steady Magnetic Field

EuCARD-2 Enhanced European Coordination for Accelerator Research & Development. Journal Publication

Characteristics and classification of plasmas

Density Fluctuation in the Tandem Mirror GAMMA 10. A. Itakura, S. Tsunoda, M. Fukuhara, H. Higaki, H. Hojo, M. Ichimura, K. Ishii,

Analytical and Experimental Studies on the Hybrid Fault Current Limiter Employing Asymmetric Non-Inductive Coil and Fast Switch

Electron cyclotron resonance plasma enhanced direct current sputtering discharge with magnetic-mirror plasma confinement

UHF Magnet Development at MIT

Lecture #2 Design Guide to Superconducting Magnet

Transcription:

Mini-RT Plasma Production and Levitation Experiments of a High-temperature Superconductor Coil in a Mini-RT Internal Coil Device Junji MORIKAWA, Kotaro OHKUNI, Dan HORI, Shigeo YAMAKOSHI, Takuya GOTO, Yuichi OGAWA Nagato YANAGI* and Toshiyuki MITO* Synopsis: Plasma is produced using a 2.45 GHz microwave in a Mini-RT internal coil device, where a high-temperature superconductor is employed. The radius of the internal coil is.15 m and its weight is 16.8 kg. The maximum coil current is 5 ka, and the typical magnetic field strength at the internal coil is.1 T. First plasma experiments were carried out using a mechanically supported coil, and a typical plasma density in the range of 1 16 m -3 was produced. When the internal coil current is decreased to less than 1 ka, plasma cannot be produced because of the disappearance of the electron cyclotron resonance layer of the 2.45 GHz microwave. Concerning to the levitation experiments of the internal coil, the coil position is monitored with laser sensors, and the levitation coil current is feedback-controlled. The HTS coil has been levitated for a period of one hour with an accuracy of 1 micrometers. Plasma production with a floating coil has been successfully initiated. Keywords: internal coil device, HTS conductor, plasma production, magnetic levitation, feedback control Mini-RT 2 K 5 ka Mini-RT Received April 16, 24 The University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan 59-5292 322-6 National Institute for Fusion Science, 322-6 Oroshi-cho, Toki, Gifu 59-5292, Japan E-mail: morikawa@ppl.k.u-tokyo.ac.jp Mini-RT 2.8 kw 2.45 GHz 2.45 GHz Mini-RT 3 Fig. 1 Mini-RT 2.45 GHz 875 G.875 T 5 ka 1 ka 514 ka Fig. 2.1 T 2.45 GHz 39 5 24 29

Fig.1 Magnetic configuration of the Mini-RT device. (a) Icoil = 5 ka (b) Icoil = 14 ka Fig. 2 Magnetic configuration for (a) Icoil =5 ka and (b) Icoil = 14 ka. The magnetic field strength is also depicted. 875 G 5 mm 5 ka 875 G 14 ka 875 G 1 ka 875 G 2.45 GHz 43 ka 428 Fig. 3 1 A 7 1 ka 23 A Mini-RT 7 Fig. 4 Mini-RT 12 kw 5 1 3 6 57 Mini-RT ECH.5.5 Pa.3 Pa.3 Pa 21 16 m -3.1% Mini-RT Mini-RT 3 Mini-RT 2 K Fig. 3 Fig. 3 Decay of the coil current and increase in coil temperature. 21 J. Cryo. Soc. Jpn. Vol. 39 No. 5 (24)

Fig.4 Plasma produced by a 2.45 GHz microwave. The internal coil is mechanically supported. 2.6 kw 51 16 m -3 2.45 GHz 71 16 m -3 Fig. 5 36 ka.2 Pa 12 W 24 mm Mini-RT n e (1 16 m -3 ) 1 5 2 1 -(56) s.1% 1-6 s.1 Pa 1-4 s Mini-RT 197.1 mm 3-4) LDX 6) Mini-RT 197 Fig. 6 6 X YZ XYZ Z 5 Z XY XY Tilt( x, y) Vertical(Z-axis) Sliding(Sx, Sy) Internal Coil 2 25 3 35 4 45 Major Radius (mm) 1 Fig. 5 Electron density and temperature profile. T e (ev) Fig. 6 Six freedoms of the floating coil 39 5 24 211

5 1 5 Fig. 7 3 2 5 5 LK- 5 (LK- 25) 35 mm1 mm 69 nm 1 µm 3 P1-P3 Fig. 8 3 P 3 P 2 P 1 Levitation coil Laser sensor Vacuum vessel Fig. 8 Top view of the Mini-RT vacuum vessel. A levitation coil and a laser sensor are located at the top of the vacuum vessel. Fig. 9 16.8 kg 5 ka Levitation coil current (ka) S 9 S Fig. 7 Laser sensors for detecting five freedoms of the floating coil. Fig. 9 Levitation coil current as a function of the distance between two coils (i.e., floating and levitation coils) for various levitation coil radii. The major radius, the coil current and the weight of the floating coil are,.15m, 1kA and 16.8 kg, respectively. The marks circle, squareand triangleare denoted to the levitation coil radius of 25 cm, 2 cm and 15 cm, respectively. 212 J. Cryo. Soc. Jpn. Vol. 39 No. 5 (24)

Z(a.u.) 2.5 2 1.5 1 2 1.5 tilt instability floating coil : R1,z Unstable Stable Lcoil Fcoil Hz PID Proportional-Integral-Differential 5 5 XY PID.5 1 1.5 2 2.5 1 2 R(a.u.) Fig. 1 Position between floating (F) and levitation (L) coils. Fig. 1 Fcoil Z= Lcoil 2.8 cm Z=28 cm Fig. 1 35 cm 5 ka 15.3 ka 1.54 Hz 4 FB-RT FB-RT Fig. 11 FB-RT Table 1 Field-Cooling FB-RT 3 4 Fig. 11 Set-up of a feedback control experiment with a miniature HTS coil. Table 1 Parameters of FB-RT miniature HTS coil. Inner / Outer Diameter 77 / 94.5 mm Number of Turns 44 Winding Method Double Pancake Inductance.272 mh Cable Type Ag-sheathed Bi-2223 Coolant Liquid Nitrogen Weight (including LN2) 296 g (321 g) 39 5 24 213

Position (m) 2 3m Fig. 12 t=.1 sec 2 d ~ z m 2 dt d dt d i i dm ( z) dz F L z ~ z L i M ( z) i F F L mg L i M z) i R i e (1) (2) L L ( (3) F L L dt mg irl FL M(z) e O z z ~ z ~ ~ if if if il il il PID e K ~ z K v~ K ~ ~ zdt K i (4) z v I Time (sec) Fig. 12 A floating coil position. The dynamic response of the coil position is studied by changing the reference position of the floating coil at t =.1 sec. L L Mini-RT 3 Fig. 13 Fig. 14 Coil support Floating coil Center stack Fig. 13 A floating HTS coil. The coil position is detected with three laser sensors, and the levitation coil current is feedback-controlled. Fig. 14 Position and current of a floating coil and a levitation coil current. The floating coil position is artificially changed at t = 5 min. The levitation coil current is gradually increased because the floating coil current is decreasing. 214 J. Cryo. Soc. Jpn. Vol. 39 No. 5 (24)

Fig. 14 t = 5 min 5 mm 1 1 m 5 g HTS HTS 69 nm H-alpha Fig. 15 Fig. 1 Fig. 14 Mini-RT 2.45 GHz 1 16 m -3 1-2 ev 1 m 1 Mini-RT m 1 1) N. Yanagi, et al. : Excitation test results of the HTS floating coil for the Mini-RT project, IEEE Trans. Appl. Supercond. 13 (23) 154-157 2) Y. Ogawa, et al.: Construction and operation of an internal coil device with a high temperature superconductor, J. Plasma Fusion Res. 79 (23) 643-644 3) J. File, et al.: J. Appl. Phys. 39 (1968) 2623 4) S. Skellett : CLM-P427 (1975) 5) S. Yoshikawa: Experiments on plasma confinement in internal-ring devices, Nucl. Fusion 13 (1973) 433-449 6) J.H. Schultz, et al.: The Levitated Dipole Experiment (LDX) magnet system, IEEE Trans. Appl. Supercond. 9 (1999) 378-381 7) J. Morikawa, et al. : Levitation experiment using a high-temperature superconductor coil for a plasma confinement device, Jpn. J. Appl. Phys. 4 (21) L129-L131 Fig. 15 Plasma produced by 2.45 GHz microwave at the condition that the HTS coil is floating. 39 5 24 215

216 J. Cryo. Soc. Jpn. Vol. 39 No. 5 (24)