• 제목/요약/키워드: KSTAR.

검색결과 303건 처리시간 0.02초

Discharge Characteristics of a KSTAR NBI Ion Source

  • Chang Doo-Hee;Oh Byung-Hoon
    • Nuclear Engineering and Technology
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    • 제35권3호
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    • pp.226-233
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    • 2003
  • The discharge characteristics of a prototype ion source was investigated, which was developed and upgraded for the NBI (Neutral Beam Injection) heating system of KSTAR (Korea Superconducting Tokamak Advanced Research). The ion source was designed for the arc discharge of magnetic bucket chamber with multi-pole cusp fields. The ion source was discharged by the emission-limited mode with the control of filament heating voltage. The maximum ion density was 4 times larger than the previous discharge controlled by a space-charge-limited mode with fully heated filament. The plasma (ion) density and arc current were proportional to the filament voltage, but the discharge efficiency was inversely proportional to the operating pressure of hydrogen gas. The maximum ion density and arc current were obtained with constant arc voltage ($80{\sim}100V$), as $8{\times}10^{11}cm^{-3}$ and 1200 A, respectively. The estimated maximum beam current was about 35 A, extracted by the accelerating voltage of 80kV.

DESIGN OF A BENDING MAGNET FOR THE KSTAR NBI SYSTEM

  • In, Sang-Ryul;Yoon, Byeong-Joo;Kim, Beom-Yeol
    • Nuclear Engineering and Technology
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    • 제38권8호
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    • pp.793-802
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    • 2006
  • The design concept of a bending magnet to be installed in the KSTAR NBI system is presented. It is the function of a bending magnet that removes unconverted ions from the main beam stream and produces an 8 MW, 120 keV deuterium neutral beam. In order to determine the proper size and shape of the bending magnet, a parametric study on the B-field pattern was carried out by changing the dimensions of the pole face model. In addition, the detailed trajectories of the dominant ion species produced in the beam line were calculated. The electrical and cooling parameters of the coil assembly were also estimated.

DISTRIBUTED CONTROL SYSTEM FOR KSTAR ICRF HEATING

  • Wang, Son-Jong;Kwak, Jong-Gu;Bae, Young-Dug;Kim, Sung-Kyu;Hwang, Churl-Kew
    • Nuclear Engineering and Technology
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    • 제41권6호
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    • pp.807-812
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    • 2009
  • An ICRF discharge cleaning and a fast wave electron heating experiment were performed. For automated operation and providing the diagnostics of the ICRF system, the ICRF local network was designed and implemented. This internal network provides monitoring, RF protection, remote control, and RF diagnostics. All the functions of the control system were realized by customized DSP units. The DSP units were tied by a local network in parallel. Owing to the distributed feature of the control system, the ICRF local control system is quite flexible to maintain. Developing the subsystem is a more effective approach compared to developing a large controller that governs the entire system. During the first experimental campaign of the KSTAR tokamak, the control system operated as expected without any major problems that would affect the tokamak operation. The transmitter was protected from harmful over-voltage events through reliable operation of the system.

KSTAR 전류인입선 및 헬륨냉매 제어시스템 제작 및 설치 (Construction and Assembly of KSTAR Current Leads and the Helium Control System)

  • 송낙형;우인식;이영주;곽상우;방은남;이근수;김정수;장용복;박현택;홍재식;박영민;김양수;최창호
    • 한국진공학회지
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    • 제16권5호
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    • pp.388-396
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    • 2007
  • KSTAR (Korea Superconducting Tokamak Advanced Research) 전류인입선(CL; Current Lead)은 4.5 K의 저온에서 운전되는 초전도 버스라인과 300 K의 실온에서 운전되는 MPS (Magnet Power Supply)를 전기적으로 연결하는 장치이다. 초기 플라즈마 발생시험을 위하여 TF (Toroidal Field) 및 PF (Poloidal Field) 리드박스에 전류인입선이 설치된다. TF 자석용 CL은 17.5 kA급 4 개의 CL에 최대 35 kA의 DC 전류가 인가되며, PF 자석용은 13 kA급 14 개의 CL에 350초간 $20\;{\sim}\;26\;kA$의 펄스 전류가 인가된다. 각각의 전류인입선은 TF 및 PF 자석에 전류를 인가하기 위한 버스라인이 연결되어 있으며, 전류인입선을 통해 초전도 버스라인으로 전달되는 전도열 및 전류인가시 발생되는 주울(Joule) 열을 차단하기 위한 헬륨냉매 제어시스템이 KSTAR 주장치와는 별도로 설치되어 있다. 리드박스 내 외부의 배관 및 제어시스템 설치완료 후 고진공 배기, 헬륨 누설검사, 전류인입선 유량 검사 및 액체질소 냉각시험을 실시하여 장치의 성능검증을 완료하였다.

Thermal and Stress Analysis of The Faraday Shield in KSTAR ICH System

  • Yoon, B.J.;Han, J.M.;Jeong, S.H.;Yoon, J.S.;Hong, B.G.
    • 한국원자력학회:학술대회논문집
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    • 한국원자력학회 1998년도 춘계학술발표회논문집(2)
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    • pp.935-940
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    • 1998
  • The Korea Superconducting Tokamak Research (KSTAR) tokamak will have 6 MW of radio-frequency (rf) heating in the ion cyclotron range of frequencies (ICRF). The response of the antenna to the heat loads is analyzed and the resulting stresses in the Faraday shield during the normal operation is calculated. Various heat loading conditions including in the analyzes are the heat loads from the plasma, the ripple-trapped beam particles and the rf loss.

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Fusion cafe - KSTAR에 숨어있는 놀라운 이야기 - KSTAR, 우주(진공도 10$^{-9}$mbar)를 품다 -

  • 국가핵융합연구소
    • 핵융합뉴스레터
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    • 통권42호
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    • pp.15-15
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    • 2009
  • 우리나라 최초의 위성 '우리별 1호'가 떠있는 곳, 지상에서 1,300km 상공의 우주는 '고진공' 상태이다. '진공'이라 함은 보통 아무것도 없는 공간을 말하지만 실제로 우주에서조차도 입자가 전혀 없는 절대진공 상태는 불가능하다. 단지 공간 안에 포함되어 있는 기체분자의 수에 따라 진공을 구분하게 되는데 '우리별 1호'가 있는 우주공간은 10$^{-9}$mbar의 고진공 상태이다. 그렇다면 지구에서도 이런 우주의 진공도를 구현해 낼 수 있을까?

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ICRF Wave Propagation and Absorption on KSTAR Plasma

  • Ju, M.H.;Hong, B.G.;Han, J.M.;Mau, T.K.
    • 한국원자력학회:학술대회논문집
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    • 한국원자력학회 1997년도 춘계학술발표회논문집(2)
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    • pp.583-588
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    • 1997
  • For the efficient current drive, the structure of ICRF wave propagation and absorption in a tokamak plasma should be first investigated. In this paper, two dimensional study on FWCD as well as ICRF minority ion heating for the KSTAR [Korea Superconducting Tok Amak Research] [1] plasma was performed using the full wave code of TORIC [2]. The ICRF wave propagation and absorption structures, the competitive power absorption between electrons and ions and the coupling of antenna/plasma are investigated.

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KSTAR 토카막 RF 안테나의 부하와 VSWR

  • 한장민;주명희;최현정;홍봉근
    • 한국원자력학회:학술대회논문집
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    • 한국원자력학회 1997년도 춘계학술발표회논문집(2)
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    • pp.577-582
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    • 1997
  • KSTAR 토카막$^1$플라즈마의 전류구동을 위한 RF 안테나 설계시 최적 조건을 2차원 파동 코드와 안테나 모듀울(module)을 이용하여 연구하였다 최적 조건을 얻기 위해 플라즈마와 안테나 매개변수 각각에 대한 부하와 전압정재파비(VSWR)의 관계를 살펴보았다. 계산결과로부터, 송전선의 특성저항 $R_{c}$=50$\Omega$, 안테나 폴로이달(poloidal) 길이 $A_{pl}$ =1.0m, 안테나 사이의 간격 $w_{d}$=4$^{0}$ 근처에서 최적의 안테나 조건을 갖음을 알 수 있었다.

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