The level of thermal noise in a resonant vibrating beam gyroscope is lower, the longer the beam. A limitation on the length of the beam arises from the consideration that the beam acts as a mechanical bandpass filter transmitting the signal being measured (the instantaneous rate of rotation) from the drive axis to the sense axis. A longer beam vibrates at a lower frequency and has a narrower resonance. The length that is acceptable depends on the bandwidth of the time variation of angular rate, which in turn, depends on the nature and mission of the vehicle that uses the gyroscope for inertial navigation. High rates of maneuvering indicate millimeter scale gyroscopes that are realized as micro-electro-mechanical devices. In the case of General Aviation, considerations of noise, as well as cost, favor a centimeter scale device.

1.
Katz, A., 1997, Computational Rigid Vehicle Dynamics, Krieger, Malabar, FL, pp. 57–58, 65.
2.
Hurty, W. C., and Rubinstein, M. F., 1964, Dynamics of Structures, Prentice Hall, Englewood Cliffs, NJ, pp. 198–203.
3.
Meirovich, L., 1975, Elements of Vibration Analysis, McGraw-Hill, NY, pp. 39–45.
4.
Nyquist
,
H.
,
1928
, “
Thermal Agitation of Electric Charge in Conductors
,”
Phys. Rev.
,
32
, pp.
110
113
.
5.
Callen
,
H. B.
, and
Welton
,
T. H.
,
1951
, “
Irreversibility and Generalized Noise
,”
Phys. Rev.
,
83
, No.
1
, pp.
34
40
.
6.
Callen
,
H. B.
, and
Greene
,
R. F.
,
1952
, “
On a Theorem of Irreversible Thermodynamics
,”
Phys. Rev.
,
86
, No.
5
, pp.
702
710
.
7.
Callen
,
H. B.
, and
Greene
,
R. F.
,
1952
, “
On a Theorem of Irreversible Thermodynamics, II
,”
Phys. Rev.
,
88
, No.
6
, pp.
1387
1391
.
8.
Gabrielson
,
T. B.
,
1993
, “
Mechanical-Thermal Noise in Micromachined Acoustic and Vibration Sensors
,”
IEEE Trans. Electron Devices
,
40
, No.
5
, pp.
903
909
.
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