首页> 外文会议>Symposium Gyro Technology; 20040921-22; Stuttgart(DE) >Bias Errors in Fiber-Optic Gyroscopes Caused by Lyot Depolarizers
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Bias Errors in Fiber-Optic Gyroscopes Caused by Lyot Depolarizers

机译:由Lyot去极化器引起的光纤陀螺仪的偏置误差

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Fiber optic gyroscopes (FOG) are by now commercially produced, nevertheless these sensors sometimes show bias errors, i.e. the offset rotation rate varies with temperature and other environmental parameters. An optical bias error source will be described, which may occur in every FOG with a Lyot depolarizer and an integrated optics circuit (IOC). Simulations deliver insight into the processes and illustrate the dependencies. Experimental results confirm the theoretical predictions very well. Usually low coherence light sources like superluminescent diodes are used in FOGs to avoid undesirable interferences between error signals from reflections etc.. Multipath propagation in the sensor takes place. The resulting path differences between the occurring light waves and their polarization determine whether they interfere or not. The analysis of the standard FOG design leads to the identification of a bias error source which has not been described yet. Although high precision FOGs usually use a polarization maintaining coil, the part in front of the IOC is in most cases made of single mode fiber to avoid a costly polarization maintaining coupler. The remaining birefringence of the single mode fiber is temperature dependent and can lead to signal fading at the IOC which acts as a polarizer. For this reason a Lyot depolarizer is introduced behind the light source to reduce the degree of polarization. The index of refraction of the IOC is different from that of the fiber so that Fresnel reflections at the interfaces occur. To reduce those the front and back face are angled polished. Due to the angle the already reduced reflections from the two divided beams additionally possess an optical path difference. But if this path difference matches the path differences gained in the depolarizer within the coherence length a rotation rate equivalent modulated phase is produced. The simulations have been carried out with an advanced simulation tool for modeling the light propagation in interferometric fiber optic sensors with low coherence light sources. Underlying is a refined method which takes polarization and coherence effects into account. The light source parameters are represented by the power spectrum resp. the coherence function. All signals and perturbations and interferences between them are considered with the corresponding degree of coherence. Active phase modulation in the FOG is modeled, too. The parameters of the incorporated materials and components like the fiber are taken into account as a function of temperature so that a full temperature dependent model of the FOG can be built. Simulation results of the errors to expect will be shown. Measurements with our fiber optic gyro show temperature dependent bias errors of up to 20/h compared to bias variations of less than 0.1/h without depolarizer. Methods to avoid this problem are addressed.
机译:光纤陀螺仪(FOG)现已商业化生产,尽管如此,这些传感器有时仍会显示偏差误差,即偏移转速随温度和其他环境参数而变化。将描述一个光学偏置误差源,该误差源可能会在具有Lyot消偏器和集成光学电路(IOC)的每个FOG中出现。通过仿真可以深入了解流程并说明相关性。实验结果很好地证实了理论预测。通常在FOG中使用诸如超发光二极管之类的低相干光源,以避免来自反射等的误差信号之间产生不希望的干扰。传感器中会发生多径传播。所产生的光波之间的路径差及其偏振决定了它们是否干涉。通过对标准FOG设计的分析,可以确定尚未描述的偏置误差源。尽管高精度FOG通常使用偏振保持线圈,但在大多数情况下,IOC前面的部分由单模光纤制成,以避免昂贵的偏振保持耦合器。单模光纤的剩余双折射取决于温度,并可能导致充当偏振器的IOC处的信号衰减。因此,在光源后面引入了Lyot消偏振器,以降低偏振度。 IOC的折射率不同于光纤的折射率,因此会在界面处发生菲涅耳反射。为了减少这些磨损,正面和背面要进行斜角抛光。由于该角度,来自两个分开的光束的已经减少的反射另外具有光程差。但是,如果该路径差与相干长度内在去偏振器中获得的路径差匹配,则会产生转速等效调制相位。使用先进的仿真工具进行了仿真,以对具有低相干光源的干涉式光纤传感器中的光传播进行建模。底层是一种考虑极化和相干效应的改进方法。光源参数由功率谱表示。相干函数。考虑所有信号,它们之间的干扰和干扰以及相应的相干程度。 FOG中的有源相位调制也已建模。考虑到所掺入的材料和组件(如纤维)的参数随温度的变化,因此可以建立FOG的完整温度相关模型。将显示预期误差的仿真结果。使用我们的光纤陀螺仪进行的测量显示,与温度相关的偏差误差高达20 / h,而没有去偏振器的偏差偏差小于0.1 / h。解决避免该问题的方法。

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