Study on Parameter Drift Mechanism of a Quartz Accelerometer with a System Analysis Method

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A publication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 33, 2013 Guest Editors: Enrico Zio, Piero Baraldi Copyright 2013, AIDIC Servizi S.r.l., ISBN 978-88-95608-24-2; ISSN 1974-9791 The Italian Association of Chemical Engineering Online at: www.aidic.it/cet DOI: 10.3303/CET1333003 Study on Drift Mechanism of a Quartz Accelerometer with a System Analysis Method Ying Chen a, Bingdong Liu a, Rui Kang a, Zebing Hou*,b a School of Reliability and Systems Engineering, Beihang University, Xueyuan Road, Haidian District, Beijing, China, 100191 b 31st Insititute, China Aerospace Science & Industry Corporation, Yungang Road, Fengtai District, Beijing, China, 100074 lbd1989@126.com A quartz accelerometer is a chief sensitive device of the inertial navigation system. However, there exists parameter during the process of transportation, storage or in work condition, which has a bad influence on the navigation accuracy. In this article, a system analysis method, the combination of FTA (Fault Tree Analysis) and FMEA (Failure Mode and Effects Analysis), is conducted to study the parameter mechanism of a quartz accelerometer and the conclusion is drawn that the mechanism mainly lies in the homogenization effect of vibration on welding. Finally, FEA (Finite Element Analysis) simulation is perceived to confirm the homogenization effect and demonstrates the correctness of the analysis results. 1. Introduction A quartz accelerometer is a chief sensitive device of the inertial navigation system, which can be used to measure the linear acceleration of the object and further to obtain its trajectory, including the speed and distance. Due to the impact of materials, variation of manufacturing process, its parameter such as scale factor s during the process of transportation, storage or in work condition, which has a bad influence on the navigation accuracy. At home and abroad the studies on parameter of a quartz accelerometer mainly focus on the mathematical modelling and the compensation of the various parameters identified by the system identification methods. Theodore (1971) has given the static error formula of an accelerometer through the test data fitting method. Fuhrman (1977) has given a method of obtaining the characteristic curve of the accelerometer to estimate the deviation of the scale factor and zero bias. Cline (1982) has used the time-constant interference equation to analyse the deviation of the inertial navigation system and clearly demonstrated the importance of choosing the proper coordinate frame for specifying shaping filters to model instrument error sources. Meskin and Itzhack (1992) have presented a new method for developing INS (Inertial Navigation System) error models which also puts all the known models in the framework and shows the equivalence among them and the method is based on several choices which uniquely define the error model. Linear error models have been presented and discussed and their eigenvalues have been computed in several special cases (Itzhack and Berman, 1987). Tiejun Qu etal (2006) has improved a self-compensation algorithm for of platform inertial navigation system and a simulation example has demonstrated the efficiency of the proposed approach. The dynamic separation method of inertial navigation instrument error during the missile's flight phase has been studied, the transfer model of inertial navigation instrument error has been analysed systemically and the SINS /Global Positioning System (GPS) Kalman filter for error separation has been designed (Gang Li etal, 2010). In this article a system analysis method of combing FTA and FMEA is conducted to study the internal and external factors that have an influence on the parameter of the quartz accelerometer and reveal the mechanism of the parameter, so as to lay the foundation for improvement of design and control of process. First of all, FTA method is used to find out the structural parameters that associated with scale factor according to its working principle. Then FMEA method is employed with regard to the assembling process to Please cite this article as: Chen Y., Liu B., Kang R., Hou Z., 2013, Study on parameter mechanism of a quartz accelerometer with a system analysis method, Chemical Engineering Transactions, 33, 13-18 DOI: 10.3303/CET1333003 13

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account, the effects on the structure by vibration lie in the homogenization of the assembling process residual stress. There are two kinds of assembling process used among the quartz accelerometer, welding process and cementation process. As is shown in Figure 3, the quartz components and coil skeleton, the soft magnet and magnetic steel, the soft magnet and isolation ring, the isolation ring and shell, are all assemble by cementation process, while the soft magnet and pre-load ring are assembled by laser spot welding. 2:Isolation ring 3:Shell Welding region 4:Pre-load ring 1:Quartz components 5:Coil skeleton 7:Soft magnet 6:Magnetic steel Figure 3: schematic diagram of assembling With regard to the assembling process under vibration, FMEA is carried out and the results are shown in Table 1. Table 1: FMEA results regarding to the assembling process under vibration Assembling Assembling Destabilizing Effects on Mechanism influenced parts process factors structure of effects structural factors 1 and 5 Cementation, l in cementation 6 and 7 Cementation 4 and 7 Welding Welding 2 and 7 Cementation 2 and 3 Cementation in cementation in welding in cementation in cementation Effects on scale factor From Table 1, it can be seen that vibration can homogenize the cementation and welding, which cause the relating structural parameters to change, thus leading the parameter. In fact, vibration has less influence on cementation than welding. Therefore, the parameter mechanism of quartz accelerometer under vibration mainly lies in its homogenization effect on welding. 16

4. FEA simulation FEA simulation is conducted to demonstrate the homogenization effect of vibration on welding. In order to simplify the problem, only half of the quartz flexible accelerometer is modelled. Figure 4 shows the finite element mesh created on the weld component. The weld position was accurately represented with fine mesh. In the finite element mesh, radial direction is the welding direction and direction Z is the through thickness direction which is also vibration direction. Figure 4: finite element model of welding region Figure 5: before and after vibration In the simulation, the welding process is simulated firstly to get welding distribution and then vibration is exerted to see the change of distribution. From the Figure 5, Figure 6 and Figure 7, it can be obviously obtained that the after vibration is reduced and homogenized than that before vibration, indicating the homogenization effect of vibration on welding. Figure 6: distribution before vibration Figure 7: distribution after vibration 5. Conclusion In this article, a system analysis method, the combination of FTA and FMEA, is used to study on parameter mechanism of a quartz accelerometer and FEA simulation is perceived to demonstrate the correctness of the analysis results. The conclusion can be drawn from the analysis and the simulation that the parameter mechanism of a quartz accelerometer under vibration mainly lies in its homogenization effect on welding, which lays the foundation for further study on improvement of design and control of process References Cline TB., 1982, A time-invariant error model for a space-stable inertial navigation system. Proceedings of the AIAA Guidance and Control, 266-276 (San Diego, CA, August. 9-11). Fuhrman TA., 1977, An improved technique for estimating accelerometer linearity from multipoint data. AIAA Guidance and Control Conference, New York, 530-547. 17

Gang Li, Yong Xian, Minghai Wang, 2010, Dynamic separation method of strap-down inertial navigation instrument error. Control and Decision Conference (CCDC), Xuzhou, May 26-28, 4302-4305. Itzhack B., Berman NIY., 1987, Control theoretic approach to inertial navigation systems. AIAA Guidance, Navigation and Control Conference, Monterey, CA, Aug. 17-19, p. 1442-1453. Meskin DG., Itzhack Y.B., 1992, Unified approach to inertial navigation system error modelling. Journal of Guidance, Control and Dynamics. 15(3),:648-652 Theodore C.M., 1971, An improved method for accelerometer precision centrifuge test data reduction. J. Spacecraft, 8(6):686-688. Tiejun Qu, Xudong Yang, Ziyun Tian, 2006, A self-compensation algorithm for of platform inertial navigation system. 1st International Symposium on Systems and Control in Aerospace and Astronautics, Harbin, Jan. 19-21. 4pp.-104. 18