The Schilowsky Gyroscope

Relativity Gyroscope Experiment ( B ) : Gyroscope Development

The central element of the Stanford relativity experiment is a cryogenic gyroscope with a performance in space many orders of magnitude superior to that of conventional earth-boiind devices. In the early pllases of the program, a great deal of thought wa? given t o the problem of achieving the performance goal, and an entirely new gyro concept was developed by William Fairbank and Francis Everi...

The Stanford Relativity Gyroscope Experiment (C): London Moment Readout of the Gyroscope

Fiber Optic Gyroscope

This paper describes the development of Fiber Optic Gyroscope (FOG) for Space applications at LEOS. The sensor has all solid-state optical devices for the precise measurements of mechanical rotation. The basic phenomenon underlying optical rotation sensing is known as the Sagnac effect. In the Sagnac effect two identical light beams traveling in opposite directions around a closed loop path exp...

The Basics of MEMS IMU/Gyroscope Alignment

Sensor misalignment is often a key consideration for high performance motion control systems that use MEMS inertial measurement units (IMUs) in their feedback loops. For the gyroscopes in the IMU, sensor misalignment describes the angular difference between each gyroscope’s axis of rotation and the system defined inertial reference frame, also known as the global frame. Managing the impact that...

The First Frequency - Modulated ( FM ) Pitch Gyroscope †

In this work, the mechanical design and the experimental validation of a microelectromechanical frequency-modulated (FM) pitch gyroscope are presented. The proposed device is fabricated through the ThELMA © surface micromachining process of STMicroelectronics and it represents, to the authors’ knowledge, the first small-footprint (690 μm × 946 μm) prototype of FM gyroscope able to measure an in...