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Upon frequency multiplication by a factor
N, the vibrational frequency fv is unaffected, as it is an
external influence. The peak frequency
change due to vibration, Df, however, becomes
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f = (A) Nf0.
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The modulation index is therefore
increased by the factor N. Expressed
in decibels, frequency multiplication by a factor N increases the phase noise
by 20 log N. When exposed to the same
vibration, the relationship between the vibration-induced phase noise of two
oscillators with the same vibration sensitivity and different carrier
frequencies is
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LB(f) = LA(f) +20 log
(fB/fA),
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where LA(f) is the
sideband level, in dBc/Hz (or dBc for sinusoidal vibration), of the
oscillator at frequency fA and LB(f) is the
sideband level of the oscillator at frequency fB. For the same acceleration sensitivity,
vibration frequency and output frequency, the sidebands are identical,
whether the output frequency is obtained by multiplication from a lower
frequency or by direct generation at the higher frequency. For example, when a 2 x 10-9/g
sensitivity 5 MHz oscillator’s frequency is multiplied by a factor of 315 to
generate a frequency of 1575 MHz, its output will contain vibration-induced
sidebands which are identical to those of a 1575 MHz SAW oscillator that has
the same 2 x 10-9/g sensitivity.
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R. L. Filler,
"The Acceleration Sensitivity of Quartz Crystal Oscillators: A Review," IEEE Transactions on
Ultrasonics, Ferroelectrics, and Frequency Control, Vol. 35, No. 3, pp.
297-305, May 1988.
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J. R. Vig, C.
Audoin, L. S. Cutler, M. M. Driscoll, E. P. EerNisse, R. L. Filler, R. M.
Garvey, W. L. Riley, R. C. Smythe, and R. D. Weglein, "Acceleration,
Vibration and Shock Effects - IEEE Standards Project P1193," Proc. 1992
IEEE Frequency Control Symposium, 763-781, 1992; also, The Effects of
Acceleration on Precision Frequency Sources, U. S. Army Laboratory
Command Research and Development Technical Report SLCET-TR-91-3, March 1991,
AD-A235470.
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