Bulletin of the Seismological Society of America
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Bulletin of the Seismological Society of America; August 1997; v. 87; no. 4; p. 1078-1080
© 1997 Seismological Society of America
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Frequency response of a strainmeter

Cinna Lomnitz

Instituto de Geofisica, UNAM National University of Mexico, 04510 Mexico, D.F.

Abstract

The amplification of a strainmeter is frequency dependent. As the wavelength {lambda} approaches the length L of the strainmeter, the amplitude vanishes, because the two extremes of the strainmeter are in phase. The sign of the response is inverted at zero crossings such that {lambda} = L/n, n = 1, 2,.... Between L < {lambda} < 2L, the amplitude of an incoming signal may be reduced by 60% or more. Filtering of the output may worsen the problem. Thus, strainmeters may be poorly suited for certain research purposes, including surface-wave studies and first-motion studies. The output of long-base strainmeters sited on low-velocity materials (such as the 732-m-long strainmeters at Piñon Flat Observatory) may require correction for amplitude distortion.




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