Blame view

Instrument/AMDA/Helios2/MAG.xml 3.04 KB
b51d3376   Elena.Budnik   helios
1
2
3
4
5
6
7
8
9
<?xml version="1.0" encoding="UTF-8"?>
<Spase xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns="http://www.spase-group.org/data/schema" xsi:schemaLocation="http://www.spase-group.org/data/schema http://www.spase-group.org/data/schema/spase-2_2_6.xsd">
  <Version>2.2.6</Version>
  <Instrument>
    <ResourceID>spase://CDPP/Instrument/AMDA/Helios2/MAG</ResourceID>
    <ResourceHeader>
      <ResourceName>MAG</ResourceName>
      <AlternateName>Helios Magnetometers : E2, E3</AlternateName>
      <ReleaseDate>2018-10-20T21:10:13Z</ReleaseDate>
4987ad03   Elena.Budnik   typo
10
      <Description>E2 : The Förster probe experiment E2 is a three component-vector magnetometer. Its purpose is to
b51d3376   Elena.Budnik   helios
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
continuously observe the interplanetary magnetic field in a frequency range up to 4 Hz. Thereby certain
phenomena are to be analysed as a function of the distance from the sun e.g. the spiral structure and
discontinuities. The measurement ranges are ± 100 nT and ± 400 nT. The resolution is ± 0.2 nT and ±
0.8 nT respectively.

For accurate measurements of the zero offset of each sensor the component parallel to the spinaxis can
be flipped by 90°. Depending on telemetry format and bitrate the digital data are fed into a time average
computer or directly connected to telemetry. A shock identification-computer triggers the S/C core
memory in case of discontinuities with variations of the ambient magnetic field magnitude.

The Förster probe experiment E2 is a three-axe vector magnetometer. It is used for the continuous
observation of the interplanetary magnetic field in a frequency range from 0 to 4 Hz. This will be
investigated phenomena such as the spiral structure and discontinuities as a function of the distance
from the Sun. The measuring ranges are ± 100 nT and ± 400 nT with a resolution of ± 0.2 nT or ± 0.8 nT.
The component that is parallel to the axis of the spin, to perform precise zero point provisions of each
sensor is rotated 90 degrees. Depending on format and bit rate digital data pass through an average
computer or directly to the telemetry. A shock wave identification computer triggers the S/C core memory
in the presence of discontinuities with magnetic field variations.

E3 :  The Rome‐GSFC magnetic field experiment utilized a triaxial fluxgate (saturable inductor) 
magnetometer.  
        </Description>
b51d3376   Elena.Budnik   helios
33
34
35
36
37
38
39
40
       <Contact>      
        <PersonID>spase://CDPP/Person/Musmann</PersonID>
        <Role>PrincipalInvestigator</Role>
      </Contact>
      <Contact>      
        <PersonID>spase://CDPP/Person/Mariani</PersonID>
        <Role>PrincipalInvestigator</Role>
      </Contact>
4987ad03   Elena.Budnik   typo
41
        <Contact>
b51d3376   Elena.Budnik   helios
42
43
44
45
46
47
48
49
50
51
52
53
54
        <PersonID>spase://SMWG/Person/Norman.F.Ness</PersonID>
        <Role>PrincipalInvestigator</Role>
      </Contact>
      <Contact>      
        <PersonID>spase://CDPP/Person/F.M.Neubauer</PersonID>
        <Role>PrincipalInvestigator</Role>
      </Contact>  
    </ResourceHeader>
    <InstrumentType>FluxGateMagnetometer</InstrumentType>
    <InvestigationName/>
    <ObservatoryID>spase://CDPP/Observatory/AMDA/Helios2</ObservatoryID>
  </Instrument>
</Spase>