1975
DOI: 10.1111/j.1365-246x.1975.tb07044.x
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Guide to the Interpretation of Crustal Refraction Profiles

Abstract: Using the reflectivity method, synthetic, vertical-component seismograms have been computed for simple velocity transitions appropriate to crustal models. Record sections of the synthetic seismograms including refracted and reflected phases aid in elucidating the fine structure of the crust since they illustrate the effects of various velocity models. The computed record sections indicate the importance to interpretation of secondary arrivals such as near-vertical incidence and wide-angle reflections and illus… Show more

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Cited by 85 publications
(33 citation statements)
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References 30 publications
(36 reference statements)
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“…5). This reflection pattern might be caused by an alternating layering of basaltic rocks and sediments, volcaniclastic material or pillow lavas (Inoue et al, 2008), which can amplify amplitudes for certain frequencies due to constructive wave interference (Braile and Smith, 1975). We therefore interpret the upper crust as an inter-layered basalt-sediment sequence.…”
Section: The Northern Edificementioning
confidence: 93%
“…5). This reflection pattern might be caused by an alternating layering of basaltic rocks and sediments, volcaniclastic material or pillow lavas (Inoue et al, 2008), which can amplify amplitudes for certain frequencies due to constructive wave interference (Braile and Smith, 1975). We therefore interpret the upper crust as an inter-layered basalt-sediment sequence.…”
Section: The Northern Edificementioning
confidence: 93%
“…Braile and Smith (1975) show that compressional wave amplitudes in a critical region (e.g., Region A) can be increased by replacing a first-order discontinuity with a gradient. They also demonstrate that a low amplitude head wave (e.g., Region E) can be produced by introducing a negative velocity gradient below the interface.…”
Section: Comparison Of Source Wavelets For Synthetics Wavelet a Is Amentioning
confidence: 98%
“…The type of head wave that is observed up to teleseismic distances is typically described as a sum of whispering gallery or interference waves which travel in the mantle lid between the Moho and the low-velocity zone of the upper mantle [e.g., Menke and Richards, 1980]. Attenuation behavior of such waves is generally quite complicated and different from the behavior of pure head waves, and the amplitudes will depend on the velocity gradient in the uppermost mantle [Hill, 1973;Braile and Smith, 1975]. Because of these complications, we do not attempt to formally model the Sn attenuation but try to determine the broad variations of the propagation efficiency.…”
Section: Methodsmentioning
confidence: 99%