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Journal ArticleDOI

Measurement of rise times of seismic pulses in rock

D. P. Blair
- 01 Jul 1982 - 
- Vol. 47, Iss: 7, pp 1047-1058
TLDR
In this paper, a model for a general system transfer function is proposed to estimate the effect of a system's impulse response on the measurement of seismic pulses in the presence of an impulsive source, which is then obtained by convolving the system impulse response with the given seismic pulse.
Abstract
Rise times for seismic pulses in rock are discussed for both nearly constant Q (NCQ) and constant Q (CQ) theories of pulse attenuation. The frequency content of the NCQ pulse is examined in detail. Frequencies close to the megahertz region are shown to have a significant contribution to the rise time of pulses a meter or so from an impulsive source. Hence, the measurement of such rise times is significantly influenced by the frequency response of the measurement system itself. In giving a numerical assessment of the system influence, I propose a model for a general system transfer function. The effect of such a system on the measurement of rise times of seismic pulses is then obtained by convolving the system impulse response with the given seismic pulse. For even the most broad‐band seismic measurement systems presently available, rise time measurements made especially within 10 m or so of an impulsive source show a large contribution dependent upon the rise time of the measurement system itself.

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Citations
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Journal ArticleDOI

Attenuation of explosion‐generated pulse in rock masses

TL;DR: In this paper, an alternative method of estimating pulse attenuation is presented, which overcomes the difficulties inherent in the rise time law, which makes no allowance for the spectral characteristics of the source except by assigning a value of tau/sub 0/ to each source.
Journal ArticleDOI

Determination of Seismic‐Wave Attenuation By Complex Trace Analysis

TL;DR: In this article, a new method to estimate seismic-wave attenuation is presented on the basis of complex trace analysis, where the effect of the dispersion, which is always associated with attenuation, can either be taken into account or can be disregarded by application of the method to the autocovariance functions of the wavelets.
Journal ArticleDOI

Experimental comparison between spectral ratio and rise time techniques for attenuation measurement

TL;DR: In this article, a relation between rise time τ and the ratio travel time to quality factor T/Q was derived using the linear relation τ=τ+C*T/Q.
Journal ArticleDOI

Injection-induced Microseismicity in Colorado Shales

TL;DR: In this paper, a number of fluid injection operations was undertaken at this site and the associated microseismicity was detected using two three-component geophones and fifteen hydrophones.
Journal ArticleDOI

Seismic pulse assessment of the changing rock mass conditions induced by mining

TL;DR: In this paper, a series of high frequency seismic pulse transmission experiments were conducted over the period when conditions in the assessed volume of rock were changing and the alteration in the rock mass conditions was induced by the general mining process (underground sites) or by controlled blasting (surface site).
References
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Journal ArticleDOI

Constant Q-wave propagation and attenuation

TL;DR: In this article, a linear model for attenuation of waves is presented, with Q, or the portion of energy lost during each cycle or wavelength, exactly independent of frequency, where wave propagation is completely specified by two parameters, e.g., Q and c0, a phase velocity at an arbitrary reference frequency ω 0.
Journal ArticleDOI

Anelastic degradation of acoustic pulses in rock

TL;DR: In this paper, a simple empirical relationship between the pulse rise time, τ and the time of propagation of a pulse, t: τ=τ0+C ∫ ) TQ-1dt where τ0 is the initial rise time (at t = 0), Q is the anelastic parameter which may be expressed in terms of the fractional loss of energy per cycle of a sinusoidal wave, Q = 2π(ΔE/E)-1, and is assumed to be essentially independent of frequency, and C is a constant whose value we estimate
Journal ArticleDOI

Ultrasonic P and S wave attenuation in dry and saturated rocks under pressure

TL;DR: In this paper, the attenuation of a rock sample relative to a high Q standard of identical geometry using Fourier spectral ratios was determined by measuring the sample attenuation relative to the standard.