• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

用于抑制频率分裂的半球形谐振器等效底角的仿真与优化

Simulation and Optimization of Hemispherical Resonator's Equivalent Bottom Angle for Frequency-Splitting Suppression.

作者信息

Gao Zhiyong, Wang Shang, Wang Zhi, Ding Xukai

机构信息

School of Fundamental Physics and Mathematical Sciences, Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences (UCAS), Hangzhou 310012, China.

University of Chinese Academy of Sciences, Beijing 101408, China.

出版信息

Micromachines (Basel). 2023 Aug 29;14(9):1686. doi: 10.3390/mi14091686.

DOI:10.3390/mi14091686
PMID:37763849
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10534843/
Abstract

As an inertial sensor with excellent performance, the hemispherical resonator gyro is widely used in aerospace, weapon navigation and other fields due to its advantages of high precision, high reliability, and long life. Due to the uneven distributions of material properties and mass of the resonator in the circumferential direction, the frequencies of the two 4-antinodes vibration modes (operational mode) of resonator in different directions are different, which is called frequency splitting. Frequency splitting is the main error source affecting the accuracy of the hemispherical resonator gyro and must be suppressed. The frequency splitting is related to the structure of the resonator. For the planar-electrode-type hemispherical resonator gyro, in order to suppress the frequency splitting from the structure, improve the accuracy of the hemispherical resonator gyro, and determine and optimize the equivalent bottom angle parameters of the hemispherical resonator, this paper starts from the thin shell theory, and the 4-antinodes vibration mode and waveform precession model of the hemispherical resonator are researched. The effect of the equivalent bottom angle on the 4-antinodes vibration mode frequency value under different boundary conditions is theoretically analyzed and simulated. The simulation results show that the equivalent bottom angle affects the 4-antinodes vibration mode of the hemispherical resonator through radial constraints. The hemispherical resonator with mid-surface radius R=15 mm and shell thickness h=1 mm is the optimization object, and the stem diameter and fillet radius R1 are experimental factors, with the 4-antinodes vibration mode frequency value and mass sensitivity factor as the response indexes. The central composite design is carried out to optimize the equivalent bottom angle parameters. The optimized structural parameters are: stem diameter D=7 mm, fillet radii R1=1 mm, R2=0.8 mm. The simulation results show that the 4-antinodes vibration mode frequency value is 5441.761 Hz, and the mass sensitivity factor is 3.91 Hz/mg, which meets the working and excitation requirements wonderfully. This research will provide guidance and reference for improving the accuracy of the hemispherical resonator gyro.

摘要

半球谐振陀螺作为一种性能优异的惯性传感器,因其具有高精度、高可靠性和长寿命等优点,在航空航天、武器导航等领域得到了广泛应用。由于谐振器材料特性和质量在圆周方向上分布不均匀,谐振器在不同方向上的两种四波腹振动模式(工作模式)的频率不同,这被称为频率分裂。频率分裂是影响半球谐振陀螺精度的主要误差源,必须加以抑制。频率分裂与谐振器的结构有关。对于平面电极式半球谐振陀螺,为了从结构上抑制频率分裂,提高半球谐振陀螺的精度,并确定和优化半球谐振器的等效底角参数,本文从薄壳理论出发,研究了半球谐振器的四波腹振动模式和波形进动模型。理论分析并模拟了等效底角在不同边界条件下对四波腹振动模式频率值的影响。模拟结果表明,等效底角通过径向约束影响半球谐振器的四波腹振动模式。以中面半径R = 15 mm、壳厚h = 1 mm的半球谐振器为优化对象,以杆径和圆角半径R1为实验因素,以四波腹振动模式频率值和质量灵敏度因子为响应指标。采用中心复合设计对等效底角参数进行优化。优化后的结构参数为:杆径D = 7 mm,圆角半径R1 = 1 mm, R2 = 0.8 mm。模拟结果表明,四波腹振动模式频率值为5441.761 Hz,质量灵敏度因子为3.91 Hz/mg,很好地满足了工作和激励要求。本研究将为提高半球谐振陀螺的精度提供指导和参考。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/0961f5ec68d2/micromachines-14-01686-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/7935f358c0e4/micromachines-14-01686-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/3e3b34dc8e77/micromachines-14-01686-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/cf270c5f1c5a/micromachines-14-01686-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/a97bd63acd07/micromachines-14-01686-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/7f5b0c147c7f/micromachines-14-01686-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/83f11be22a03/micromachines-14-01686-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/99325af3e40c/micromachines-14-01686-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/1de9133df03a/micromachines-14-01686-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/dd8724073eda/micromachines-14-01686-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/2d73605dd543/micromachines-14-01686-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/886a16c19139/micromachines-14-01686-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/0c848b18b7a4/micromachines-14-01686-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/0961f5ec68d2/micromachines-14-01686-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/7935f358c0e4/micromachines-14-01686-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/3e3b34dc8e77/micromachines-14-01686-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/cf270c5f1c5a/micromachines-14-01686-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/a97bd63acd07/micromachines-14-01686-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/7f5b0c147c7f/micromachines-14-01686-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/83f11be22a03/micromachines-14-01686-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/99325af3e40c/micromachines-14-01686-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/1de9133df03a/micromachines-14-01686-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/dd8724073eda/micromachines-14-01686-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/2d73605dd543/micromachines-14-01686-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/886a16c19139/micromachines-14-01686-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/0c848b18b7a4/micromachines-14-01686-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fac/10534843/0961f5ec68d2/micromachines-14-01686-g013.jpg

相似文献

1
Simulation and Optimization of Hemispherical Resonator's Equivalent Bottom Angle for Frequency-Splitting Suppression.用于抑制频率分裂的半球形谐振器等效底角的仿真与优化
Micromachines (Basel). 2023 Aug 29;14(9):1686. doi: 10.3390/mi14091686.
2
Research of Frequency Splitting Caused by Uneven Mass of Micro-Hemispherical Resonator Gyro.微半球谐振陀螺质量不均匀引起的频率分裂研究。
Micromachines (Basel). 2022 Nov 18;13(11):2015. doi: 10.3390/mi13112015.
3
Frequency split elimination method for a solid-state vibratory angular rate gyro with an imperfect axisymmetric-shell resonator.用于具有非理想轴对称壳体谐振器的固态振动角速率陀螺仪的频率分裂消除方法。
Sensors (Basel). 2015 Feb 2;15(2):3204-23. doi: 10.3390/s150203204.
4
Scanning measurement of surface error and thickness variation of the hemispherical resonator.半球形谐振器表面误差和厚度变化的扫描测量。
Appl Opt. 2022 Oct 1;61(28):8435-8445. doi: 10.1364/AO.467742.
5
The Synthesis Model of Flat-Electrode Hemispherical Resonator Gyro.平面电极半球谐振陀螺的综合模型。
Sensors (Basel). 2019 Apr 9;19(7):1690. doi: 10.3390/s19071690.
6
Areal measurement of vibration modes of a hemispherical shell resonator by deflectometry.通过偏转测量法对半球形壳谐振器振动模式进行面积测量。
Appl Opt. 2022 Jun 1;61(16):4919-4926. doi: 10.1364/AO.456744.
7
The Influence of Nonlinear High-Intensity Dynamic Processes on the Standing Wave Precession of a Non-Ideal Hemispherical Resonator.非线性高强度动态过程对非理想半球形谐振器驻波进动的影响
Sensors (Basel). 2024 Apr 24;24(9):2709. doi: 10.3390/s24092709.
8
Research on bell-shaped vibratory angular rate gyro's character of resonator.关于钟形振动角速率陀螺的谐振器特性的研究。
Sensors (Basel). 2013 Apr 10;13(4):4724-41. doi: 10.3390/s130404724.
9
Standing Wave Binding of Hemispherical Resonator Containing First-Third Harmonics of Mass Imperfection under Linear Vibration Excitation.线性振动激励下含质量缺陷一次至三次谐波的半球形谐振器的驻波束缚
Sensors (Basel). 2020 Sep 23;20(19):5454. doi: 10.3390/s20195454.
10
The Energy Compensation of the HRG Based on the Double-Frequency Parametric Excitation of the Discrete Electrode.基于离散电极双频参量激励的心率计能量补偿
Sensors (Basel). 2020 Jun 23;20(12):3549. doi: 10.3390/s20123549.

本文引用的文献

1
Research of Frequency Splitting Caused by Uneven Mass of Micro-Hemispherical Resonator Gyro.微半球谐振陀螺质量不均匀引起的频率分裂研究。
Micromachines (Basel). 2022 Nov 18;13(11):2015. doi: 10.3390/mi13112015.
2
Standing Wave Binding of Hemispherical Resonator Containing First-Third Harmonics of Mass Imperfection under Linear Vibration Excitation.线性振动激励下含质量缺陷一次至三次谐波的半球形谐振器的驻波束缚
Sensors (Basel). 2020 Sep 23;20(19):5454. doi: 10.3390/s20195454.