The HRG makes use of a small thin solid-state hemispherical shell, anchored by a thick stem. This shell is driven to a flexural resonance by dedicated electrostatic forces generated by electrodes which are deposited directly onto separate
fused quartz structures that surround the shell. For a single-piece design (i.e., the hemispherical shell and stem form a monolithic part) made from high-purity
fused quartz, it is possible to reach a
Q factor of over 30-50 million in vacuum, thus the corresponding
random walks are extremely low. The Q factor is limited by the coating (extremely thin film of gold or platinum) and by fixture losses. Such resonators have to be fine-tuned by ion-beam micro-erosion of the glass or by
laser ablation in order to be perfectly dynamically balanced. When coated, tuned, and assembled within the housing, the Q factor remains over 10 million. In application to the HRG shell,
Coriolis forces cause a
precession of vibration patterns around the
axis of rotation. It causes a slow precession of a
standing wave around this axis, with an angular rate that differs from input one. This is the
wave inertia effect, discovered in 1890 by British scientist
George Hartley Bryan (1864–1928). Therefore, when subject to rotation around the shell symmetry axis, the standing wave does not rotate exactly with the shell, but the difference between both rotations is nevertheless perfectly proportional to the input rotation. The device is then able to sense rotation. The electronics which sense the standing waves are also able to drive them. Therefore, the gyros can operate in either a "whole angle mode" that sense the standing waves' position or a "force rebalance mode" that holds the standing wave in a fixed orientation with respect to the gyro. Originally used in space applications (attitude and orbit control systems for spacecraft), HRG is now used in advanced
inertial navigation systems, in
attitude and heading reference systems, and
HRG gyrocompasses. ==Advantages==