| Literature DB >> 26999153 |
Fei Yu1, Chongyang Lv2, Qianhui Dong3.
Abstract
Owing to their numerous merits, such as compact, autonomous and independence, the strapdown inertial navigation system (SINS) and celestial navigation system (CNS) can be used in marine applications. What is more, due to the complementary navigation information obtained from two different kinds of sensors, the accuracy of the SINS/CNS integrated navigation system can be enhanced availably. Thus, the SINS/CNS system is widely used in the marine navigation field. However, the CNS is easily interfered with by the surroundings, which will lead to the output being discontinuous. Thus, the uncertainty problem caused by the lost measurement will reduce the system accuracy. In this paper, a robust H∞ filter based on the Krein space theory is proposed. The Krein space theory is introduced firstly, and then, the linear state and observation models of the SINS/CNS integrated navigation system are established reasonably. By taking the uncertainty problem into account, in this paper, a new robust H∞ filter is proposed to improve the robustness of the integrated system. At last, this new robust filter based on the Krein space theory is estimated by numerical simulations and actual experiments. Additionally, the simulation and experiment results and analysis show that the attitude errors can be reduced by utilizing the proposed robust filter effectively when the measurements are missing discontinuous. Compared to the traditional Kalman filter (KF) method, the accuracy of the SINS/CNS integrated system is improved, verifying the robustness and the availability of the proposed robust H∞ filter.Entities:
Keywords: Krein space theory; SINS/CNS integrated system; missing measurements; robust H∞ filter; uncertainty problem
Year: 2016 PMID: 26999153 PMCID: PMC4813971 DOI: 10.3390/s16030396
Source DB: PubMed Journal: Sensors (Basel) ISSN: 1424-8220 Impact factor: 3.576
Figure 1Schematic diagram of the SINS/CNS integrated system.
Simulation parameters.
| Parameters | Values |
|---|---|
| initial latitude | |
| initial longitude | |
| initial velocity | |
| gravity acceleration | |
| initial misalignment angles | |
| constant drifts of the gyroscopes | |
| random noise of the gyroscopes | |
| constant biases of the accelerometers | |
| random noise of the accelerometer | |
| sampling frequency | 98 Hz |
Figure 2The estimated errors of the misalignment angles when .
Figure 3The estimated errors of the misalignment angles when .
Comparisons of the running times.
| Running Time (s) | ||
|---|---|---|
| Kalman Filter | Proposed Filter | |
Figure 4Schematic of the experimental setup.
Figure 5The IMU (left) and GPS (right) used in the experiments.
Main parameters of the SINS and star sensor.
| Sensors | Parameters | Values |
|---|---|---|
| Gyro | Dynamic range | |
| Bias stability | ||
| Random walk | ||
| Scale factor stability | ||
| Accelerometer | Dynamic range | |
| Bias stability | ||
| Random walk | ||
| Scale factor stability | ||
| Star Sensor | Field of view | |
| Attitude accuracy | ||
| Data update frequency | 20 Hz |
Figure 6The horizontal angle errors with the normal Kalman filter method and the proposed robust filter. The blue dash line indicates the horizontal errors by utilizing the normal Kalman filter method; The green solid line indicates the horizontal errors by utilizing the novel method proposed in this article.
Figure 7The azimuth angle errors with the normal Kalman filter method and the proposed robust filter. The blue dash line indicates the azimuth errors by utilizing the normal Kalman filter method; The green solid line indicates the azimuth errors by utilizing the novel method proposed in this article.