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  <Version>2.0.0</Version>
  <Instrument>
    <ResourceID>spase://SMWG/Instrument/AE-C/RPA</ResourceID>
    <ResourceHeader>
      <ResourceName>Retarding Potential Analyser/Drift Meter (RPA)</ResourceName>
      <AlternateName>RPA</AlternateName>
      <ReleaseDate>2019-05-05T12:34:56Z</ReleaseDate>
      <Description>This experiment was designed to determine vector ion drift velocities, ion concentration and
   temperature, and spacecraft potential. An ionospheric irregularity index was also obtained from the ion
   concentration sensor. The experiment consisted of a retarding potential analyzer with four planar sensor
   heads. The sensor head used for ion drift measurements was co-located with another head, and all were spaced
   nearly equally, looking outward from the satellite equator. Since the satellite spin axis was perpendicular
   to the orbit plane, these heads could observe along the spacecraft velocity vector in either the spin or
   despun mode of the spacecraft. The primary objective of this experiment was to provide accurate ion
   temperatures with other measurements being of secondary importance. Three of the sensor heads were similar.
   They had two grounded entrance grids, two retarding grids, a suppressor grid, a shield grid, and a collector.
   A linear sweep voltage (32 or 22 to 0 V, up or down) was normally applied to the retarding grids in 0.75 s.
   Interpretation of the resulting current-voltage profiles provided the ion temperature, the ion and electron
   concentration, some ion composition information, vehicle potential and plasma drift velocity parallel to
   the velocity vector. Two of the three similar sensors had an additional grid between the entrance and
   retarding grids in order to protect inner grids from ion bombardment during electron measurements. The
   other significant feature of these two sensors was that a small positive collector bias could be applied
   to assure adequate access of thermal electrons to the collector. With the retarding grid at constant zero
   volts, current changes could be observed for 3-s periods to obtain gradients of ion concentration.
   Electron parameters were measured in a manner similar to ions. Ions in mass ranges 1 to 4, 14 to 16, 24 to 32
   and greater than 40 atomic mass units could be identified. The fourth sensor head was for the ion-drift
   velocity measurements, and consisted of four grounded grids, a negatively biased suppressor grid, and a
   four-segment collector. Differences in various collector segment currents provided ion-drift directional
   component information. More details of this experiment are available in
   W. B. Hanson et al., Radio Sci., v. 8, n. 4, p. 333, 1973. NSSDC has all the useful data that exist
   from this investigation.</Description>
      <Contact>
        <PersonID>spase://SMWG/Person/William.B.Hanson</PersonID>
        <Role>PrincipalInvestigator</Role>
</Contact>
      <InformationURL>
        <Name>NSSDC's Master Catalog</Name>
        <URL>https://nssdc.gsfc.nasa.gov/nmc/experiment/display.action?id=1973-101A-04</URL>
        <Description>Information about the Retarding Potential Analyser/Drift Meter (RPA) experiment on the AE-C mission.</Description>
</InformationURL>
   <InformationURL>
        <Name>Radio Science Journal Article</Name>
        <URL>https://onlinelibrary.wiley.com/doi/abs/10.1029/RS008i004p00333</URL>
        <Description>Detailed information about the Retarding Potential Analyser/Drift Meter (RPA) experiment on the AE-C mission.</Description>
</InformationURL>
</ResourceHeader>
    <InstrumentType>RetardingPotentialAnalyser</InstrumentType>
    <InvestigationName>Retarding Potential Analyser/Drift Meter (RPA) on AE-C</InvestigationName>
    <ObservatoryID>spase://SMWG/Observatory/AE-C</ObservatoryID>
</Instrument>
</Spase>
