共查询到19条相似文献,搜索用时 281 毫秒
1.
2.
3.
在EASTICRF天线中,法拉第屏蔽是ICRF天线中的一个非常重要的部件。实验时,它位于真空室内直接面对等离子体,将承受着很大的热负荷。基于EASTICRF天线法拉第屏蔽结构的安全性,本文利用有限元的方法,首先对热负荷最大的法拉第屏蔽冷却管道在不同水流速下进行热分析,考察在不同水流速工况下法拉第屏蔽冷却管道上的温度分布情况,再通过热 结构耦合方法对法拉第屏蔽冷却管道进行结构分析,了解法拉第屏蔽在不同水流速下的应力大小和分布情况,分析结果为未来EASTICRF天线实验提供理论指导。另外,对法拉第屏蔽冷却管道结构进行了优化改进,并对优化改进后的法拉第屏蔽冷却管道在相同工况下进行了热和热 结构分析,分析结果确定了优化改进后的法拉第屏蔽冷却管道结构的优越性,分析数据为未来法拉第屏蔽冷却管道的优化改进提供理论指导,分析方法为其他同类装置提供有益的参考。 相似文献
4.
在全超导托卡马克核聚变实验装置(EAST)上进行核聚变试验时,离子回旋共振加热(ICRF)是该试验过程中加热等离子体的主要方法之一,而对发射机、传输线、真空室以及天线中的重要参数进行实时监测是托卡马克装置中ICRF对等离子体进行功率耦合的重要保障。提供了一种采用FPGA的ICRF实时监控系统设计方案、AD9252芯片以及SN74LS14型号施密特触发器进行数据采样,实现对各故障信号的实时显示、报警以及信号源的及时切断,同时利用FPGA可重复编程的特点,便于后期对系统进行维护和升级。 相似文献
5.
6.
7.
中国聚变工程实验堆(China Fusion Engineering Test Reactor,CFETR)的增殖包层采用多模块的设计方案,即在环向和极向上由多个包层模块组成。当发生等离子体大破裂或垂直位移事件等电磁工况时,增殖包层上感应产生的巨大电磁载荷将共同作用于背板结构上,严重影响增殖系统的结构稳定性。为了研究增殖包层极向分块对背板电磁载荷分布的影响,使用通用有限元软件ANSYS,实现了一个具有36 ms指数电流猝灭的等离子大破裂工况模拟。首先系统评估了采用U型套管方式的氦冷陶瓷增殖(Helium Cooled Ceramic Breeder,HCCB)包层模块上的电磁力和力矩分布。然后详细比较不同极向分块形式对包层扇段电磁载荷分布的影响。研究结果表明:当高场侧包层模块位置和数目不变时,通过增加低场侧包层的极向分块数目,等离子体大破裂工况在低场侧包层上产生的电磁力和力矩均有所减少。对于高场侧包层,当低场侧包层极向分块增加时,径向方向的电磁力有稍微的增加,其他两个方向变化不明显。此外,随着极向分块数目的增加,高/低场侧包层扇段包层的总电磁力均表现出下降的趋势。 相似文献
8.
9.
通过高压气体注入的方式进行等离子体破裂缓解,已成为目前托卡马克装置破裂缓解的主要研究方向。本文介绍了等离子体破裂防护高压气体快速充气阀的工作原理,应用该快速充气阀在HT-7上进行了高压气体注入实验,并分析了其对等离子体破裂缓解的影响。实验发现,杂质气体的注入可很大程度上提高热辐射强度,降低等离子体温度;调节充气量可改变电流的猝灭率,从而可改变装置所受的电磁力负载。实验表明,该套快速充气阀可完全满足HT-7实验的需求。 相似文献
10.
在EAST装置内离子回旋共振加热(ICRF)系统中,天线与液态调配器之间传输线上的驻波电压幅值会因为负载阻抗的变化而变得很大,为此设计了ICRF功率传输预匹配支节。本设计采用解析法和Smith圆图法相结合的分析方式,在ICRF系统中安装了预匹配支节,并对其降压效果进行了测试。测试结果表明,安装预匹配支节之后,预匹配支节与液态调配器之间传输线上的驻波电压幅值得到有效降低,可作为优化ICRF功率传输系统功率传输性能的候选者。 相似文献
11.
X.Q. Yang Y.T. Song S.T. Wu Y.P. Zhao J.X. Zhang Z.W. Wang 《Fusion Engineering and Design》2012,87(7-8):1249-1252
In order to satisfy the requirements of heating plasma on EAST project, 3 MW ion cyclotron range of frequency (ICRF) heating system will be available at the second stage. Based on this requirement, the second ICRF antenna, has been designed for EAST. The antenna which is planned to operate with a frequency ranging from 30 MHz to 110 MHz, comprises four poloidal current straps. The antenna has many cooling channels inside the current straps, faraday shield and baffle to remove the dissipated RF loss power and incoming plasma heat loads. The antenna is supported via a cantilever support box to the external support structure. Its assembly is plugged in the port and fixed on the support box. External slideway and bellows allow the antenna to be able to move in the radial direction. The key components of the second ICRF antenna has been designed together with structural and thermal analysis presented. 相似文献
12.
The phased current distribution at current straps for the KSTAR ICRF antenna causes a power imbalance at each strap owing to the mutual couplings between current straps. In order to mitigate the effect of coupling, a decoupler connecting two phased feeding lines are designed based on both a lumped element antenna model and a distributed transmission line model. Though the decoupler parameter is dependent on the loading resistance, which depends on plasma condition, an analysis shows that the decoupling is effective in the wide range of loading resistance assuming the low variation of mutual inductance between straps. A circuit analysis also shows that the RF characteristics of a complex RF transmission system are matched well for the asymmetric antenna current spectrum aiming for a non-inductive current drive of KSTAR. The calibration result of decoupler after installation is also discussed. 相似文献
13.
杨宇晴 张新军 赵燕平 秦成明 程艳 毛玉周 杨桦 王健华 袁帅 王磊 琚松青 陈根 邓旭 张开 万宝年 李建刚 宋云涛 龚先祖 钱金平 张涛 《等离子体科学和技术》2018,20(4):45102-111
Recent ion cyclotron resonance frequency(ICRF) coupling experiments for optimizing ICRF heating in high power discharge were performed on EAST. The coupling experiments were focus on antenna phasing and gas puffing, which were performed separately on two ports of the ion cyclotron resonance heating(ICRH) system of EAST. The antenna phasing was performed on the I-port antenna, which consists of four toroidally spaced radiating straps operating in multiple phasing cases; the coupling performance was better under low wave number ∣k_‖∣(ranging from 4.5 to 6.5). By fuelling the plasma from gas injectors, placed as uniformly spaced array from top to bottom at each side limiter of the B-port antenna, which works in dipole phasing, the coupling resistance of the B-port antenna increased obviously.Furthermore, the coupling resistance of the I-port antenna was insensitive to a smaller rate of gas puffing but when the gas injection rate was more than a certain value(1021 s~(-1)), a sharp increase in the coupling resistance of the I-port antenna occurred, which was mainly caused by the toroidal asymmetric boundary density arising from gas puffing. A more specific analysis is given in the paper. 相似文献
14.
Gen CHEN 《等离子体科学和技术》2022,24(1):15602
The Ion Cyclotron Radio Frequency (ICRF) heating antenna on EAST adopts a decoupling device to constrain power coupling among the radiation straps, which was discovered shortcomings such as long size, poor contact, and etc. In order to improve these weak points, a new type decoupler with terminal-loaded tunable capacitor is designed to replace the previous design. Besides the capability of the tunable admittance parameters of decoupler, the withstand voltage of the capacitor is the most significant consideration for working under high power. Therefore, the theoretical analysis carefully elaborates the capacitor withstand voltage, and the detailed analytical equations and criteria for design are given. After the comparative analysis of theoretical calculation and 3D simulation results, the decoupler design scheme is finalized. The capacitor-loaded decoupler has been successfully adopted for ICRF antenna at port N on EAST, and achieved the optimization of adjacent port isolation from −22 to −58 dB at 37 MHz without plasma to restrict mutual coupling. The new design of the decoupler has greatly improved its compactness and automatic adjustment performance, and could be good solution for the decoupling network of ICRF antennas. 相似文献
15.
Analysis and design of the Alfven wave antenna system for the SUNIST spherical tokamak are presented. Two candidate antenna concepts, folded and unfolded, are analyzed and compared with each other. In the frequency range of Alfven resonance the impedance spectrums of both two concept antennas for major modes are numerically calculated in a 1-D MHD framework. The folded concept is chosen for engineering design. The antenna system is designed to be simple and requires least modification to the vacuum vessel. The definition of the antenna shape is guided by the analyses with constraints of existing hardware layouts. Each antenna unit consists of two stainless steel straps with a thickness of 1 mm. A number of boron nitride tiles are assembled together as the side limiters for plasma shielding. Estimation shows that the structure is robust enough to withstand the electromagnetic force and the heat load for typical discharge duty cycles. 相似文献
16.
17.
V. Kyrytsya P. Dumortier F. Louche A. Messiaen M. Vervier 《Fusion Engineering and Design》2011,86(6-8):901-904
Each of the two ITER ICRF antennas consists of a close-packed array of 24 straps arranged in a 6 poloidal by 4 toroidal array. Three poloidally adjacent straps (a “triplet” of straps) are fed together through a 4-port junction from one 20 Ohm feeding line. The complete array has to radiate 20 MW of RF power over a frequency range of 40 MHz to 55 MHz and for different toroidal phasings. The RF optimization of the antenna has been performed numerically on one triplet of straps (1/8th of the antenna) [1], [2]. In parallel a number of reduced-scale mock-ups of one triplet of the ITER ICRH antenna were constructed in order to validate the results of the numerical optimization [1], [3].The aim of this work is primarily to benchmark the CST MWS® [4] numerical modeling against numerous measurements done on the mock-up of the 2007 design. Moreover MWS calculates the 3D distribution of the currents and of the fields of the triplet. Hence it gives the possibility to check the fields and current distributions resulting from the optimisation study of the ITER ICRH antenna triplet done by changing geometrical parameters of the straps and antenna box of the mock-up of 2007 design [1], [2], [3]. The considered parameters are: strap width, antenna box depth and vertical septum recess with respect to the front of the current strap. The impact of the presence of the Faraday screen is also evaluated.Excellent agreement between modeled and measured S parameters is obtained. Analysis of the fields and currents distributions on the straps is reported. Excellent current balance is confirmed. 相似文献
18.
《Fusion Engineering and Design》2014,89(11):2642-2646
Radio frequency (RF) power in the ion cyclotron range of frequencies (ICRF) is one of the primary auxiliary heating techniques for Experimental Advanced Superconducting Tokamak (EAST). The ICRF system for EAST has been developed to support long-pulse high-β advanced tokamak fusion physics experiments. The ICRF system is capable of delivering 12 MW 1000-s RF power to the plasma through two antennas. The phasing between current straps of the antennas can be adjusted to optimize the RF power spectrum. The main technical features of the ICRF system are described. Each of the 8 ICRF transmitters has been successfully tested to 1.5 MW for a wide range of frequency (25–70 MHz) on a dummy load. Part of the ICRF system was in operation during the EAST 2012 spring experimental campaign and a maximum power of 800 kW (at 27 MHz) lasting for 30 s has been coupled for long pulse H mode operation. 相似文献
19.
Y.D. Bae J.G. Kwak S.J. Wang J.S. Yoon S.K. Kim C.K. Hwang B.G. Hong 《Fusion Engineering and Design》2007,82(3):307-316
A new ICRF antenna originating from the prototype antenna was constructed for the KSTAR tokamak in 2002. The performance of the antenna was experimentally estimated at the RF test stand without a plasma. Recently three series of RF tests were performed at a frequency of 30 MHz; without any cooling, with a water-cooling for only the antenna, and with a water-cooling of the antenna and the transmission line connected to the antenna. In the tests, a half of the current strap was connected to a RF source via a matching circuit with the other half one connected to an open terminated coaxial line, and the other three straps were shorted at the input ports. During the RF pulse, the temperatures at several positions of the antenna cavity wall were measured by embedded thermocouples and the temperature profile of the front face of the antenna was measured by an IR camera. The line voltage, forward and reflected powers, and the RFTC pressure were also measured. The water-cooled antenna showed several enhanced performances in a comparison with the non-cooled case, and the standoff voltage was significantly increased. By utilizing a water-cooling of the antenna and the transmission line, we achieved a standoff voltage of 41.3 kVp for a pulse length of 300 s, and we could extend the pulse length up to 600 s at a maximum voltage of 35.0 kVp without encountering any problems, which considerably exceeds the design requirements. 相似文献