期刊文献+

MEMS gyro temperature compensation identification algorithm based on thin plate spline interpolation method

MEMS gyro temperature compensation identification algorithm based on thin plate spline interpolation method
原文传递
导出
摘要 MEMS gyroscopes are widely used in the underwater vehicles owing to their excellent performance and affordable costs.However,the temperature sensitivity of the sensor seriously affects measurement accuracy.Therefore,it is significantly to accurately identify the temperature compensation model in this paper,the calibration parameters were first extracted by using the fast calibration algorithm based on the Persistent Excitation Signal Criterion,and then,MEMS gyro temperature compensation model was established by utilizing the thin plate spline interpolation method,and the corresponding identification results were compared with the results from the polynomial fitting method.The effectiveness of the proposed algorithm has been validated through the comparative experiment. MEMS gyroscopes are widely used in the underwater vehicles owing to their excellent performance and affordable costs.However,the temperature sensitivity of the sensor seriously affects measurement accuracy.Therefore,it is significantly to accurately identify the temperature compensation model in this paper,the calibration parameters were first extracted by using the fast calibration algorithm based on the Persistent Excitation Signal Criterion,and then,MEMS gyro temperature compensation model was established by utilizing the thin plate spline interpolation method,and the corresponding identification results were compared with the results from the polynomial fitting method.The effectiveness of the proposed algorithm has been validated through the comparative experiment.
出处 《Chinese Journal of Acoustics》 CSCD 2016年第4期485-496,共12页 声学学报(英文版)
  • 相关文献

参考文献4

二级参考文献26

  • 1张桂才 王巍 等.方波调制干涉式光纤陀螺中的温度相位噪声研究[J].光子学报,1999,28(23):93-98.
  • 2张桂才 王巍.环圈温度特性对光纤陀螺输出漂移的影响[J].光子学报,1999,28(1):317-324.
  • 3[1]Lrfevre H C.The Fiber-Optic Gyroscope[M].London:ARTECH HOUSE,1993.
  • 4[2]Daganais D M,Goldberg L,Moeller R P,etal.Wavelength stability characteristics of a high-power amplified superfluorescent source[J].Journal of Lightwave Technology,1999,17(8):1415-1422.
  • 5[3]Alhonse G A,Gilbert D B,Harvey M G,etal.High-power superlu-minescent diodes[J].IEEE Journal of Quantum Electronics,1988,24(12):2454-2457.
  • 6[4]Osamu Mikami,Yoshio Noguchi,Katsuaki Magari,et al.Polariza-tion insensitive superluminescent diode at 1.5 ìm with a tensile-strained-berrier MQW[J].IEEE Transactions Photenics Technology Letters,1991,4(7):703-705.
  • 7[8]Ojeda L,Chung H,Berenstein J.Precision-calibration of fiber-optics gyroscopes for mobile robot navigation[C]//Michael S Bielas,Pro-ceedings of the 2000 IEEE International Conference on Robotics & Automation,San Francisco,CA:IEEE,2000:2064-2069.
  • 8[10]Chatterjee S,Hadi A S,Price B.Regression Analysis by Example[M].Canada:John Wiley & Sons Inc,2000.
  • 9[11]Manolakis D G,Ingle V K,Kogen S M.Statistical and Adaptive Sig-nal Processing[M].USA:McGraw-Hill Education Co,2000.
  • 10LefevreHC.光纤陀螺仪[M].北京:国防工业出版社,2002.30-33.

共引文献55

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部