1990
DOI: 10.1016/0148-9062(90)90006-n
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A model of acoustic pulse propagation and its application to determine Q for a rock mass

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Cited by 14 publications
(7 citation statements)
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“…(15)). As was mentioned in the previous subsection, the value of c depends on the experimental details and on how the pulse rise time is measured (BLAIR, 1990;KAVETZKY et al, 1990). Equation (17) always remains valid, however, provided the relation between pulse rise time and Q v has the form described by eq.…”
Section: Enhanced Velocity Tomographymentioning
confidence: 99%
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“…(15)). As was mentioned in the previous subsection, the value of c depends on the experimental details and on how the pulse rise time is measured (BLAIR, 1990;KAVETZKY et al, 1990). Equation (17) always remains valid, however, provided the relation between pulse rise time and Q v has the form described by eq.…”
Section: Enhanced Velocity Tomographymentioning
confidence: 99%
“…Stronger damping of the high-frequency part of the signal spectrum can be seen as a broadening of the recorded pulse or equivalently as an increase of the pulse rise time. This broadening has been found to be related to the Q and v factors as follows (KAVETZKY et al, 1990;GLADWIN and STACEY, 1974):…”
Section: Pulse Broadening Attenuation Tomographymentioning
confidence: 99%
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“…If a pressure pulse is used as a source wavelet, then the spectrum change manifests itself in a pulse rise time broadening along a ray path. This broadening has been found to be related to the quality fac- (2) where the integral is taken along a ray path, c is some constant depended on a source characteristic (c ,• 0.5) [Blair and Spathis 1984;Kavetzky et al 1990] and to is the 'pure' source pulse rise time. Using this approach estimation of Q requires a very stable source of acoustic pulses to assure the same to and c for all source-receiver pairs.…”
Section: Enhanced Velocity Tomographymentioning
confidence: 99%