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ResourceID
spase://CNES/NumericalData/CDPP-AMDA/IMP-8/MIT/imp-mit-k0

Description

The MIT Faraday cup experiment on IMP 8 measures
currents from solar wind ions, and from these measurements we calculate
the velocity, density, and temperature of the solar wind. The IMP 8 data
files consist of fine resolution data (approximately 1 minute resolution).

        IMP 8 spins with a period of approximately 2.7s. The Faraday 

Cup (FC) instrument scans the solar wind distribution stepping through a
contiguous set of energy windows, one step per spacecraft spin. The FC
instrument divides the spin into thirty-two, 11.25 degree angular sectors
and integrates the measured currents over different angular sectors
depending upon the Mode in which the instrument is operating. The border
between two of the 11.25 degree angular sectors lies on the Sun-spacecraft
line.

        The FC sensor collector plate is divided into two, 

semi-circular halves; the division line is parallel to the spacecraft spin
plane which is approximately parallel to the ecliptic plane. The split
collector allow determination of the bulk plasma flow relative to the spin
plane; North/South angles refer to flows coming from above or below the
spin plane respectively (flows from the South are designated as having a
positive N/S angle).

        The bulk flow angle in the spin plane is determined from the 

measurements of current vs. rotation angle. The currents telemetered to
the ground are the sums of currents for the two half-collectors ("A" and
"B") and, for the TMS and AQM modes, also the current for the
half-collector "B".

        Electrons are measured except for the eight angles near the Sun.

        The experiment has two memories only one of which is operating 

perfectly. As a result, only every other TMS spectrum is usable, and the
time between spectra is usually twice that that would be expected from the
spacecraft spin rate. The bad half-memory also limits the energy windows
that can be used in the other modes, since they require both memories to
hold the data. On occasion, the data are read out rapidly enough by the
spacecraft to allow repeated use of the good half-memory, and the time
resolution in the TMS is approximately 32 seconds.

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Version:2.4.1

NumericalData

ResourceID
spase://CNES/NumericalData/CDPP-AMDA/IMP-8/MIT/imp-mit-k0
ResourceHeader
ResourceName
best fit
AlternateName
IMP 8 Solar Wind Plasma Faraday Cup Data
ReleaseDate
2013-09-11 09:48:17Z
Description

The MIT Faraday cup experiment on IMP 8 measures
currents from solar wind ions, and from these measurements we calculate
the velocity, density, and temperature of the solar wind. The IMP 8 data
files consist of fine resolution data (approximately 1 minute resolution).

        IMP 8 spins with a period of approximately 2.7s. The Faraday 

Cup (FC) instrument scans the solar wind distribution stepping through a
contiguous set of energy windows, one step per spacecraft spin. The FC
instrument divides the spin into thirty-two, 11.25 degree angular sectors
and integrates the measured currents over different angular sectors
depending upon the Mode in which the instrument is operating. The border
between two of the 11.25 degree angular sectors lies on the Sun-spacecraft
line.

        The FC sensor collector plate is divided into two, 

semi-circular halves; the division line is parallel to the spacecraft spin
plane which is approximately parallel to the ecliptic plane. The split
collector allow determination of the bulk plasma flow relative to the spin
plane; North/South angles refer to flows coming from above or below the
spin plane respectively (flows from the South are designated as having a
positive N/S angle).

        The bulk flow angle in the spin plane is determined from the 

measurements of current vs. rotation angle. The currents telemetered to
the ground are the sums of currents for the two half-collectors ("A" and
"B") and, for the TMS and AQM modes, also the current for the
half-collector "B".

        Electrons are measured except for the eight angles near the Sun.

        The experiment has two memories only one of which is operating 

perfectly. As a result, only every other TMS spectrum is usable, and the
time between spectra is usually twice that that would be expected from the
spacecraft spin rate. The bad half-memory also limits the energy windows
that can be used in the other modes, since they require both memories to
hold the data. On occasion, the data are read out rapidly enough by the
spacecraft to allow repeated use of the good half-memory, and the time
resolution in the TMS is approximately 32 seconds.

Acknowledgement
For papers and presentations using these data, please acknowledge the MIT Space Plasma Physics Group and the path through which you accessed the data.
Contacts
RolePersonStartDateStopDateNote
1.PrincipalInvestigatorspase://SMWG/Person/Alan.J.Lazarus
2.TeamMemberspase://SMWG/Person/John.D.Richardson
InformationURL
Name
Readme file at SPDF
URL
Description

Text created by MIT IMP8 plasma team

AccessInformation
RepositoryID
Availability
Online
AccessRights
Open
AccessURL
Name
CDPP/AMDA HAPI Server
URL
Style
HAPI
Description

Web Service to this product using the HAPI interface.

Format
CSV
Acknowledgement
Thank you for acknowledging the use of AMDA in publications with wording like "Data analysis was performed with the AMDA science analysis system provided by the Centre de Données de la Physique des Plasmas (CDPP) supported by CNRS, CNES, Observatoire de Paris and Université Paul Sabatier, Toulouse".. See the Rules of the road at http://amda.cdpp.eu/help/policy.html. Please acknowledge the Data Providers.
AccessInformation
RepositoryID
Availability
Online
AccessRights
Open
AccessURL
Name
CDPP/AMDA Web application
URL
Description

Access to Data via CDPP/AMDA Web application.

Format
CSV
Format
VOTable
Format
CDF
Format
PNG
Acknowledgement
Thank you for acknowledging the use of AMDA in publications with wording like "Data analysis was performed with the AMDA science analysis system provided by the Centre de Données de la Physique des Plasmas (CDPP) supported by CNRS, CNES, Observatoire de Paris and Université Paul Sabatier, Toulouse".. See the Rules of the road at http://amda.cdpp.eu/help/policy.html. Please acknowledge the Data Providers.
ProcessingLevel
Calibrated
ProviderName
NSSDC
InstrumentIDs
MeasurementType
ThermalPlasma
TemporalDescription
TimeSpan
StartDate
1973-10-31 20:10:27Z
StopDate
2006-07-26 17:10:35Z
Cadence
PT58S
ObservedRegion
Heliosphere.NearEarth
ObservedRegion
Earth.Magnetosheath
Parameter #1
Name
density
ParameterKey
imp_mit_nfit
Description

(Better, from fits) Proton number density

UCD
phys.density;phys.atmol.ionStage
Units
cm^-3
UnitsConversion
1e6>m^-3
RenderingHints
DisplayType
TimeSeries
ValidMin
0.0
ValidMax
100.0
FillValue
9999.0
Particle
ParticleType
Proton
ParticleType
Ion
Qualifier
Fit
Qualifier
Scalar
ParticleQuantity
NumberDensity
Parameter #2
Name
v_bulk
ParameterKey
imp_mit_vfit
Description

(Better, from fits) Ion Flow Velocity (aberration corrected)

UCD
phys.veloc;phys.atmol.ionStage
Units
km/s
UnitsConversion
1e3>m/s
CoordinateSystem
CoordinateRepresentation
Spherical
CoordinateSystemName
GSE
RenderingHints
DisplayType
TimeSeries
ValidMin
100.0
ValidMax
3000.0
FillValue
9999.0
Particle
ParticleType
Proton
ParticleType
Ion
Qualifier
Fit
Qualifier
Magnitude
ParticleQuantity
FlowVelocity
Parameter #3
Name
v_thermal
ParameterKey
imp_mit_vthfit
Description

(Better, from fits) Proton most-probable thermal
speed (aberration corrected). Thermal speed is the most probable thermal
speed (i.e., the square root of [2kT/m(proton)]). To convert thermal speed
to temperature in eV, multiply 0.0052 by the square of the thermal speed;
to convert to temperature [K], multiply the square of the thermal speed by
60.5.

UCD
phys.veloc;phys.atmol.ionStage
Units
km/s
UnitsConversion
1e3>m/s
RenderingHints
DisplayType
TimeSeries
ValidMin
1.0
ValidMax
500.0
FillValue
9999.0
Particle
ParticleType
Proton
ParticleType
Ion
Qualifier
Fit
Qualifier
Scalar
ParticleQuantity
ThermalSpeed
Parameter #4
Name
flow angle e/w
ParameterKey
imp_mit_velewfit
Description

(Best, from fits) Proton East/West flow angle
(aberration corrected). Azimuth is E/W, meaning bulk flow from the East
or the West side of the Sun respectively. Positive azimuth angle means
flow from the West.

UCD
pos.posAng;phys.veloc;phys.atmol.ionStage
Units
deg
CoordinateSystem
CoordinateRepresentation
Spherical
CoordinateSystemName
GSE
RenderingHints
DisplayType
TimeSeries
ValidMin
-45.0
ValidMax
45.0
FillValue
9999.0
Particle
ParticleType
Proton
ParticleType
Ion
Qualifier
Fit
Qualifier
DirectionAngle.AzimuthAngle
ParticleQuantity
FlowVelocity
Parameter #5
Name
flow angle n/s
ParameterKey
imp_mit_velnsfit
Description

(Best, from fits) Proton North/South flow angle
(aberration corrected). Azimuth is N/S, meaning bulk flow from the North
or the South side of the Sun respectively. Positive azimuth angle means
flow from the North.

UCD
pos.posAng;phys.veloc;phys.atmol.ionStage
Units
deg
CoordinateSystem
CoordinateRepresentation
Spherical
CoordinateSystemName
GSE
RenderingHints
DisplayType
TimeSeries
ValidMin
-45.0
ValidMax
45.0
FillValue
9999.0
Particle
ParticleType
Proton
ParticleType
Ion
Qualifier
Fit
Qualifier
DirectionAngle.AzimuthAngle
ParticleQuantity
FlowVelocity