R. Knight, Christopher Scheri, J. Pulskamp, R. Rudy, D. DeVoe
{"title":"大振幅线性驱动四倍质量陀螺仪","authors":"R. Knight, Christopher Scheri, J. Pulskamp, R. Rudy, D. DeVoe","doi":"10.1109/INERTIAL56358.2023.10103988","DOIUrl":null,"url":null,"abstract":"Coriolis vibratory gyroscope drive amplitude of 16 $\\upmu\\mathrm{m}$ is demonstrated with $+30$ ppm frequency shift nonlinearity. Here, MEMS quadruple mass gyroscope (QMG) mechanical flexures are specifically designed to separate spurious modes without affecting linear operation of gyroscope drive over large amplitudes. A simulated frequency change of $+480$ ppm was initially predicted, however, when electrostatically driven at large amplitudes comb drive and sense tips begin to introduce spring softening reducing nonlinearity to $+30$ ppm. Careful consideration was also taken to electrostatically tune as-fabricated frequency mismatch without further exacerbating nonlinearity. Angle random walk (ARW) versus drive amplitude is plotted with a demonstrated $8\\times$ improvement compared to similar quadruple mass gyroscopes.","PeriodicalId":236326,"journal":{"name":"2023 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-03-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Large Amplitude Linear Drive Quadruple Mass Gyroscope\",\"authors\":\"R. Knight, Christopher Scheri, J. Pulskamp, R. Rudy, D. DeVoe\",\"doi\":\"10.1109/INERTIAL56358.2023.10103988\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Coriolis vibratory gyroscope drive amplitude of 16 $\\\\upmu\\\\mathrm{m}$ is demonstrated with $+30$ ppm frequency shift nonlinearity. Here, MEMS quadruple mass gyroscope (QMG) mechanical flexures are specifically designed to separate spurious modes without affecting linear operation of gyroscope drive over large amplitudes. A simulated frequency change of $+480$ ppm was initially predicted, however, when electrostatically driven at large amplitudes comb drive and sense tips begin to introduce spring softening reducing nonlinearity to $+30$ ppm. Careful consideration was also taken to electrostatically tune as-fabricated frequency mismatch without further exacerbating nonlinearity. Angle random walk (ARW) versus drive amplitude is plotted with a demonstrated $8\\\\times$ improvement compared to similar quadruple mass gyroscopes.\",\"PeriodicalId\":236326,\"journal\":{\"name\":\"2023 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)\",\"volume\":\"17 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-03-28\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2023 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/INERTIAL56358.2023.10103988\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2023 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/INERTIAL56358.2023.10103988","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Large Amplitude Linear Drive Quadruple Mass Gyroscope
Coriolis vibratory gyroscope drive amplitude of 16 $\upmu\mathrm{m}$ is demonstrated with $+30$ ppm frequency shift nonlinearity. Here, MEMS quadruple mass gyroscope (QMG) mechanical flexures are specifically designed to separate spurious modes without affecting linear operation of gyroscope drive over large amplitudes. A simulated frequency change of $+480$ ppm was initially predicted, however, when electrostatically driven at large amplitudes comb drive and sense tips begin to introduce spring softening reducing nonlinearity to $+30$ ppm. Careful consideration was also taken to electrostatically tune as-fabricated frequency mismatch without further exacerbating nonlinearity. Angle random walk (ARW) versus drive amplitude is plotted with a demonstrated $8\times$ improvement compared to similar quadruple mass gyroscopes.