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        <identifier>oai:www.ideals.illinois.edu:2142/85100</identifier>
        <datestamp>2023-07-11</datestamp>
        <setSpec>col_2142_5131</setSpec>
        <setSpec>col_2142_14800</setSpec>
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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:contributor>Rodney Burton</dc:contributor>
          <dc:creator>Rysanek, Filip</dc:creator>
          <dc:date>2015-09-25T22:34:25Z</dc:date>
          <dc:date>2015-09-25T22:34:25Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>2007</dc:date>
          <dc:date>2007</dc:date>
          <dc:description>A pulsed vacuum arc discharge emits a plasma as well as macroparticles in the form of micron-sized molten droplets of cathode material. Due to their direction of flight and submicron to 100 mum diameter, these macroparticles often pose a contamination threat for both spacecraft-based thrusters, and thin film deposition systems. The velocity, mass and charge of copper macroparticles emitted by a 100 A arc was experimentally measured, and compared to a model based on thermionic electron emission. The macroparticle velocity was determined by using a time-of-flight velocity filter. Less than 1% of collected particles are larger than 5.7 mum, but they account for 50% of the collected mass. The charge was calculated by measuring particle deflection in a transverse electric field. The model predicts, and the experimental results verify, that the charge on the macroparticles is positive, as compared to the negative charge expected for a DC vacuum arc. Experimental results show a roughly quadratic dependence of particle charge on the particle diameter (q&amp;sim;D2), with a 1 mum particle having a positive charge of &amp;sim;1000 electronic charges (1.6 x 10-16 C), and a 5 mum particle having a charge of &amp;sim;25000 electronic charges. The model is particle temperature dependent, and gives q&amp;sim;D2 at 1750 K and q&amp;sim;D1.7 at 2200 K. Arguments are also made for limitations on particle temperature due to radiative and evaporative cooling.</dc:description>
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  Previous issue date: 2007</dc:description>
          <dc:description>Embargo set by: Seth Robbins for item 86381
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>94 p.</dc:description>
          <dc:description>Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 2007.</dc:description>
          <dc:identifier>http://hdl.handle.net/2142/85100</dc:identifier>
          <dc:identifier>(MiAaPQ)AAI3270015</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:subject>Physics, Fluid and Plasma</dc:subject>
          <dc:title>Charging of Macroparticles Ejected From a Pulsed Vacuum Arc</dc:title>
          <dc:type>text</dc:type>
          <degree>
            <department>Aerospace Engineering</department>
            <discipline>Aerospace Engineering</discipline>
            <grantor>University of Illinois at Urbana-Champaign</grantor>
            <level>Dissertation</level>
            <name>Ph.D.</name>
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