Ring Laser Gyroscopes for Inertial Navigation and Transportation Systems

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Keith Alan Wilhelm

Good information about (RLG).

Sam Goldwasser

The brief description of the RLG, above, is not quite accurate and applies more to the Fiber-Optic Gyro (FOG). Here is an arguably better one:

The ring laser gyro (RLG) consists of a solid triangular or square block of glass with a hole drilled in it parallel to each edge. Mirrors are added at each corner, a mixture of Helium-Neon gases is added, and a stable laser cavity is formed by a suitable set of 3 or 4 mirrors. The conditions are chosen to allow two counter-rotating laser beams to be established – one clockwise (CW) and the other counter-clockwise (CCW). One of the mirrors is very slightly transmitting so that the CCW and CW beams can exit the laser cavity and then be mixed together in an interferometer that senses their relative phase.

If the RLG is stationary (not rotating) with respect to its central axis, the relative phase of the two beams is constant and the detector output is constant.

If the RLG is rotated about its central axis, the CW and CCW beams will experience a phase shift in the opposite direction. Since a ring laser gyro is an active device (as opposed to a passive fiber-optic gyro) this change is phase will force a corresponding change in the optical frequency of the counter-rotating beams. The result will be a beat in the audio band called the "Sagnac frequency" that is proportional to the rotation rate. This can be measured to very high accuracy by detecting the fringes when the CCW and CW beam are combined with optics similar to those used for homodyne metrology applications, which also provide directional information. In essence, the RLG is like a rotary encoder relative to a fixed inertial frame.

That's it in a nutshell, though in practice, it's not quite that simple.