Spelling suggestions: "subject:"acoustic wave velocity"" "subject:"coustic wave velocity""
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Magneto-acoustic response of a 2D carrier systemKennedy, Ian January 1999 (has links)
No description available.
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Acoustic velocity structure of the carboneras fault zone, SE SpainTaylor, Rochelle Louise January 2013 (has links)
The Carboneras fault zone (CFZ, Almería Province, SE Spain) is a major NE-SW trending tectonic lineament that marks part of the diffuse plate boundary between Iberia and Africa. Developed within a basement terrain dominated by mica schist, the fault system comprises two main strands within a complex zone up to 1 km wide. Between these two strands is a braided network of left-lateral strike-slip, phyllosilicate-rich fault gouge bands, ranging between 1 and 20 m in thickness, passively exhumed from up to 3 km depth. The excellent exposure in a semi-arid environment, the wide range of rock types and fault structures represented and the practicality of carrying out in-situ geophysical studies makes this fault zone particularly well suited to verifying and interpreting the results of in-situ seismic investigations. Integration of elements of field study, laboratory analysis and modelling has aided interpretation of the internal structure of the fault zone. Ultrasonic measurements were made using standard equipment over confining and pore pressure ranges appropriate to the upper 10 km of the continental crust. Seismic velocities have also been approximated from modal analysis and mineral phase elastic properties and adjusted for the effects of porosity. In-situ seismic investigations recorded P-wave velocities 40-60% lower than those measured in the laboratory under corresponding pressures and at ambient temperatures for hard rock samples. Fault gouge velocities measured in the laboratory, however, are comparable to those measured in the field because, unlike the host rocks, fault gouges are only pervasively micro-fractured and lack the populations of long cracks (larger than the sample size) that cause slowing of the velocities measured in the field. By modelling the effect of fractures on seismic velocity (by superimposing upon the laboratory seismic data the effects of crack damage) the gap between field- and laboratory-scale seismic investigations has been bridged. Densities of macroscopic cracks were assessed by measuring outcrop lengths on planar rock exposures. Assuming crack length follows a power law relation to frequency, this fixes a portion of the power spectrum, which is then extrapolated to cover the likely full range of crack sizes. The equations of Budiansky and O'Connell (1976), linking crack density to elastic moduli, were used to calculate modified acoustic velocities, and the effects of the wide range of crack sizes were incorporated by breaking the distribution down into small sub-populations of limited range of crack density. Finally, the effect of overburden pressure causing progressively smaller cracks to close was incorporated to predict velocity versus depth of burial (i.e. pressure). Determination of rock physical properties from laboratory analysis and sections constructed from geological mapping provides a representation of velocity from selected parts of the Carboneras fault zone. First break tomography images show particularly well the location of steeply-inclined fault cores, and these correlate generally well with geological mapping and laboratory velocity measurements corrected for the effect of cracks. The decoration of the fault zone with intrusive igneous material is well correlated with the results of geological observations. Comparisons made between the field (seismic) inversion model and laboratory forward velocity model in El Saltador valley show the laboratory and field velocity measurements made within the fault zone can be reconciled by accounting for the effects of crack damage in field data.
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Attenuation of the higher-order cross-sectional modes in a duct with a thin porous layerHoroshenkov, Kirill V., Yin, Y. January 2005 (has links)
No / A numerical method for sound propagation of higher-order cross-sectional modes in a duct of arbitrary cross-section and boundary conditions with nonzero, complex acoustic admittance has been considered. This method assumes that the cross-section of the duct is uniform and that the duct is of a considerable length so that the longitudinal modes can be neglected. The problem is reduced to a two-dimensional (2D) finite element (FE) solution, from which a set of cross-sectional eigen-values and eigen-functions are determined. This result is used to obtain the modal frequencies, velocities and the attenuation coefficients. The 2D FE solution is then extended to three-dimensional via the normal mode decomposition technique. The numerical solution is validated against experimental data for sound propagation in a pipe with inner walls partially covered by coarse sand or granulated rubber. The values of the eigen-frequencies calculated from the proposed numerical model are validated against those predicted by the standard analytical solution for both a circular and rectangular pipe with rigid walls. It is shown that the considered numerical method is useful for predicting the sound pressure distribution, attenuation, and eigen-frequencies in a duct with acoustically nonrigid boundary conditions. The purpose of this work is to pave the way for the development of an efficient inverse problem solution for the remote characterization of the acoustic boundary conditions in natural and artificial waveguides.
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La fissuration thermique dans les roches / Thermal microcracking in rockGriffiths, Luke 23 February 2018 (has links)
Lorsqu'elle est chauffée, la roche peut subir une microfissuration thermique, qui influence ses propriétés physiques, mécaniques, thermiques, et de transport. La surveillance de la microfissuration thermique en laboratoire a été principalement réalisée pendant le chauffage, et rarement lors du refroidissement ou du chauffage cyclique que la roche subit dans les volcans et les réservoirs géothermiques. Un nouvel appareil a été élaboré pour surveiller les émissions acoustiques et mesurer les vitesses des ondes élastiques à haute température. L'état de fissuration a été évalué grâce à un nouvel algorithme d'analyse microstructurale, et l'influence des microfissures sur les propriétés des roches a été mesurée et modélisée. Selon la microstructure, la microfissuration peut avoir lieu pendant le chauffage ou le refroidissement, et les microfissures existantes peuvent s’ouvrir et se fermer de façon réversible avec des changements de température, et influencer les propriétés de la roche. / Rock may undergo thermal microcracking when heated, affecting its physical, mechanical, thermal, and transport properties. Thermal microcrack monitoring in the laboratory has mainly been performed during heating, and rarely during the cyclic heating and cooling relevant for volcanoes and geothermal reservoirs. For this, a new dedicated apparatus for the acoustic emission monitoring and wave velocity measurement at high temperatures was elaborated, building on previous designs. Microcrack damage was assessed with a new algorithm for quantitative microstructural analysis, and the influence of thermal microcracks on rock properties was measured and modelled. Depending on the rock type and initial microcrack content, microcracking occurred during either heating, cooling, or neither, and existing microcracks reversibly opened or closed with increasing temperature. In Earth's crust, the evolution of rock properties with temperature may be significant and is determined by the microstructure.
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