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        <identifier>oai:www.ideals.illinois.edu:2142/87722</identifier>
        <datestamp>2023-07-11</datestamp>
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        <thesis xmlns="http://www.ndltd.org/standards/metadata/etdms/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.ndltd.org/standards/metadata/etdms/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdms11.xsd http://purl.org/dc/elements/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdmsdc.xsd">
          <dc:description>160 p.</dc:description>
          <dc:contributor>Harris, John G.</dc:contributor>
          <dc:creator>Block, Gareth Ian</dc:creator>
          <dc:date>2015-09-28T16:23:40Z</dc:date>
          <dc:date>2015-09-28T16:23:40Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>2004</dc:date>
          <dc:date>2004</dc:date>
          <dc:description>"We devised two reciprocal experiments to study these phenomena. ""EK transmission"" occurs when an applied voltage creates an electro-acoustic wave; in practice, this leads to thermoelastic motion, as well as electrokinetics, so that we have had to account for both effects. Conversely, ""EK reception"" occurs when a pressure wave generates a measurable voltage in electrolyte-saturated sediments. The EK reception apparatus made use of a submerged, acoustic transducer to insonify a water-sediment interface with short, 50 kHz sine-wave bursts and chirped pulses from 10--800 kHz. The resulting wave motion was monitored using Ag/AgCl electrodes fixed in a vertical array above and below the sediment interface. We measured the conductivity dependence of two kinds of EK behavior: (1) voltages generated within the samples that were localized around the transmitted ""fast"" waves, and (2) electromagnetic (EM) waves produced at the water-sediment interface. Fast-wave voltages were often greater than 500 muV, while the EM-wave potentials were usually 100 muV in magnitude. A model of plane-wave reflection from a water-EK-Biot interface leads to theoretical predictions that compare very well to experimental data for sand and glass microspheres. Both EM- and fast-wave voltages are caused by relative fluid motion in the sediment, a feature that is characteristic of poroelastic media---but not predicted by either fluid or solid models."</dc:description>
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  Previous issue date: 2004</dc:description>
          <dc:description>Embargo set by: Seth Robbins for item 89003
Lift date: Forever
Reason: Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs</dc:description>
          <dc:description>Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs</dc:description>
          <dc:description>U of I Only</dc:description>
          <dc:description>Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 2004.</dc:description>
          <dc:identifier>http://hdl.handle.net/2142/87722</dc:identifier>
          <dc:identifier>(MiAaPQ)AAI3153250</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:subject>Physical Oceanography</dc:subject>
          <dc:title>Coupled Acoustic and Electromagnetic Disturbances in a Granular Material Saturated by a Fluid Electrolyte</dc:title>
          <dc:type>text</dc:type>
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            <department>Theoretical and Applied Mechanics</department>
            <discipline>Theoretical and Applied Mechanics</discipline>
            <grantor>University of Illinois at Urbana-Champaign</grantor>
            <level>Dissertation</level>
            <name>Ph.D.</name>
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