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}
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.