1mm密度干涉仪

W. Ernst, M. Goldman, F. Senk, H. Anderson, M. McCarthy, V. Arunasalam, P. Efthimion
{"title":"1mm密度干涉仪","authors":"W. Ernst, M. Goldman, F. Senk, H. Anderson, M. McCarthy, V. Arunasalam, P. Efthimion","doi":"10.1109/ICSWA.1981.9335097","DOIUrl":null,"url":null,"abstract":"A primary control diagnostic instrument on the Princeton Tokamak Fusion Test Reactor (TFTR) will be a 1mm double-pass interferometer. The interferometer will provide: (a) line average electron density measurements for densities up to 2 × 1014 cm−3, (b) a permissive signal for control of neutral beam firing, and (c) an input signal for the gas feedback controlling system that regulates the electron density level. A 1mm wavelength was selected because of the following considerations: 1. A reliable 1 watt carcinotron source is available. 2. The cut-off density for the probing frequency, 1015 cm−3, is a factor of 3 above the highest average density to be measured. 3. At 1mm wavelength refraction problems are not severe along the available horizontal mid-plane transmission path (i.e., along the density gradient). 4. Low-loss in over-sized waveguide allows the interferometer to be located remotely from the tokamak and thus minimize environmental problems. 5. The interferometer is relatively insensitive to vibration.","PeriodicalId":254777,"journal":{"name":"1981 International Conference on Submillimeter Waves and Their Applications","volume":"26 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1981-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"TFTR 1mm Density Interferometer\",\"authors\":\"W. Ernst, M. Goldman, F. Senk, H. Anderson, M. McCarthy, V. Arunasalam, P. Efthimion\",\"doi\":\"10.1109/ICSWA.1981.9335097\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A primary control diagnostic instrument on the Princeton Tokamak Fusion Test Reactor (TFTR) will be a 1mm double-pass interferometer. The interferometer will provide: (a) line average electron density measurements for densities up to 2 × 1014 cm−3, (b) a permissive signal for control of neutral beam firing, and (c) an input signal for the gas feedback controlling system that regulates the electron density level. A 1mm wavelength was selected because of the following considerations: 1. A reliable 1 watt carcinotron source is available. 2. The cut-off density for the probing frequency, 1015 cm−3, is a factor of 3 above the highest average density to be measured. 3. At 1mm wavelength refraction problems are not severe along the available horizontal mid-plane transmission path (i.e., along the density gradient). 4. Low-loss in over-sized waveguide allows the interferometer to be located remotely from the tokamak and thus minimize environmental problems. 5. The interferometer is relatively insensitive to vibration.\",\"PeriodicalId\":254777,\"journal\":{\"name\":\"1981 International Conference on Submillimeter Waves and Their Applications\",\"volume\":\"26 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1981-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1981 International Conference on Submillimeter Waves and Their Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICSWA.1981.9335097\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1981 International Conference on Submillimeter Waves and Their Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICSWA.1981.9335097","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

摘要

普林斯顿托卡马克聚变试验反应堆(TFTR)的主要控制诊断仪器将是一个1mm双通干涉仪。干涉仪将提供:(a)密度高达2 × 1014 cm−3的线平均电子密度测量,(b)控制中性束发射的允许信号,以及(c)调节电子密度水平的气体反馈控制系统的输入信号。选择1mm波长的原因如下:可靠的1瓦致癌源是可用的。2. 探测频率的截止密度为1015 cm−3,比要测量的最高平均密度高3倍。3.在1mm波长的折射问题是不严重沿可用的水平中层传输路径(即,沿密度梯度)。4. 超大尺寸波导的低损耗使干涉仪能够远离托卡马克,从而最大限度地减少环境问题。5. 干涉仪对振动相对不敏感。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
TFTR 1mm Density Interferometer
A primary control diagnostic instrument on the Princeton Tokamak Fusion Test Reactor (TFTR) will be a 1mm double-pass interferometer. The interferometer will provide: (a) line average electron density measurements for densities up to 2 × 1014 cm−3, (b) a permissive signal for control of neutral beam firing, and (c) an input signal for the gas feedback controlling system that regulates the electron density level. A 1mm wavelength was selected because of the following considerations: 1. A reliable 1 watt carcinotron source is available. 2. The cut-off density for the probing frequency, 1015 cm−3, is a factor of 3 above the highest average density to be measured. 3. At 1mm wavelength refraction problems are not severe along the available horizontal mid-plane transmission path (i.e., along the density gradient). 4. Low-loss in over-sized waveguide allows the interferometer to be located remotely from the tokamak and thus minimize environmental problems. 5. The interferometer is relatively insensitive to vibration.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信