Conference Paper

Low cost CVG for high-grade north finders and targeting systems

Authors:
  • InnaLabs Ltd
  • Collins Aerospace
  • Salience Consulting
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Abstract

Low-cost accurate orientation as required for targeting, pointing and personal navigation is generally obtained by using FOGs (Fibre Optical Gyros) and DTGs (Dynamically Tuned Gyros). When considering the alignment time and the complexity of the system, those gyros within strapdown systems have shown themselves to be particularly relevant and today numerous systems are operated this way. However, reliability and cost are still two key drivers and new applications are seeking alternatives which are more cost effective. In spite of the emergence of Vibratory Gyros Technology, as illustrated by the high grade Hemispherical Resonator Gyro (HRG), the cost for 1 mrad accuracy is still high which prevents the effective deployment across the civilian market of accurate True North-Finders (TNF) and pointing systems. INNALABS Ltd has risen to the challenge and has developed a low-cost CVG (Coriolis Vibratory Gyroscope) able to meet the market demand for low-cost accurate TNF and pointing systems. Although the INNALABS' CVG has been developed primarily for stabilisation control systems and tactical grade systems, some specific refinements of the control loop electronics are leading to few 0.01 °/hr bias stability and ARW better than 0.01 °/√hr as required for 1 mrad accuracy. Statistical data on key performance characteristics will be presented including the bias stability and the output noise. As an example of a practical implementation, the 2 position method for True North measurement will be described with a result consistent with 1 mrad heading accuracy. This underlines the capability of INNALABS' technology of branching into the TNF and the pointing market segments.

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... The MEMS accelerometer is installed on the X axis, and the gyro on the Y axis of the m-frame. Considering the gyro's bias E b , the gyro's output is expressed as: W iemy = ω ie * sin α(sin L cos θ sin γ − cos L cos φ sin γ sin θ + cos L cos γ sin φ)+ ω ie * cos α(sin L sin θ + cos L cos θ cos φ) + E b (11) where W iemy represents the gyro's output. To simplify the above formula, A and B are used: ...
... From the above Equations (11) and (12), we can see that the modulated gyroscope output is relevant to the earth rotation rate. The amplitude of the modulated signal can be used as a good verification of true north finding. ...
... Then Equations (11) and (14) can be rewritten as follows: ...
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... In recent years, vibrating sensors have become ubiquitous [1][2][3]. This is because of their simple design (no moving parts), robustness, and continuous improvements in algorithms and electronics. ...
... Despite of not being deeply addressed in the modern literature, it is one of the main obstacles in the development of inertial sensors [10,11]. In fact, in the development of the ring laser gyroscope, it was the lock-in of frequencies of two counter-rotating laser [3] beams, which posed the biggest challenge to overcome, in order to achieve a fully functional optical sensor [10]. ...
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... Following in the footsteps of these pioneers and after the launch of its tactical grade Coriolis Vibratory Gyroscopes [7] [8], InnaLabs® recently introduced the AI-Q-2010, AI-Q-1410 and AI-Q-710 Quartz Pendulous Servo Accelerometers. These Accelerometers are the latest addition to InnaLabs® quality line of high performance "built in Europe" and ITAR-Free sensors targeted at navigation, tactical, control and measurement applications. ...
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  • J Beitia