1969
DOI: 10.1111/j.1365-2478.1969.tb01992.x
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Some Experiments Concerning the Primary Seismic Pulse*

Abstract: Recordings were made with three types of detector of the primary compressional (P) and shear (S) wave pulses generated by explosions in boreholes. Charge weights varied from 0.08 kg to 9.5 kg and detector distances varied from about 3 m to about 80 m. Scaling by the simple factor WI/s, where

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Cited by 17 publications
(14 citation statements)
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References 18 publications
(16 reference statements)
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“…It implies that both the amplitude and period of far field source wavelets will scale as the cube root of the mass or the energy of the charge. O'Brien (1969) found that this law held for both primary compressional (P) and shear (S) waves for charge weights varying from 0.08 to 9.5 kg. However, O'Brien also found that the larger charges were " more efficient generators of seismic energy "-that is, a larger fraction of the initial available energy is converted into elastic radiation by larger charges.…”
Section: Of the Scaling Law For A Buried Point Sourcementioning
confidence: 92%
“…It implies that both the amplitude and period of far field source wavelets will scale as the cube root of the mass or the energy of the charge. O'Brien (1969) found that this law held for both primary compressional (P) and shear (S) waves for charge weights varying from 0.08 to 9.5 kg. However, O'Brien also found that the larger charges were " more efficient generators of seismic energy "-that is, a larger fraction of the initial available energy is converted into elastic radiation by larger charges.…”
Section: Of the Scaling Law For A Buried Point Sourcementioning
confidence: 92%
“…Since rocks are weaker in tension than in compression, the rock fails in tension and radial tension cracks are created in the permanently deformed nonlinear zone (e.g. O'Brien, 1969). Figure 1 shows the cavity, the nonlinear zone and the elastic zone.…”
Section: Theorymentioning
confidence: 99%
“…In the spectral ratio of the seismograms, the spectrum of the earth impulse response cancels, to give the ratio of the source spectra. A well‐known scaling relationship of the source time function and the cube root of the explosive energy (Werth and Herbst, 1963; O’Brien, 1969) allows the two source time functions to be found. This scaling does not take account of realistic differences in physical properties of the rock at the two source locations, however, and is not sufficient to explain all the observed differences in the seismograms.…”
Section: Introductionmentioning
confidence: 99%
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“…In a homogeneous rock stratum, the wavelet is influenced by the structure and physiomechanical characteristics of the rock; it is also affected by the excitation factors of the seismic source, such as the nature and charge weight of the explosives, the depth of the excitation well, and charging constitution [8][9][10][11][12]. To date, theoretical calculation methods for the relation between explosion parameters and the seismic source wavelet are limited in number [13,14], and studies in this respect have long been heavily relying on field experiments [8,12,[15][16][17]. However, field experiments cost high.…”
Section: Introductionmentioning
confidence: 99%