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SPASE version 2.0.1
Solar wind magnetic field and plasma data at 1-min resolution created from IMP 8 data shifted to the Earth's bow shock nose (BSN).
We acknowledge A.Szabo and R. Lepping of the MAG team, A. Lazarus of the PLS team and J. King and N. Papitashvili of NASA/SPDF and ADNET who created this product.
| Role | Person | |
|---|---|---|
| 1. | Data producer | Dr. Joseph H. King |
| 2. | Data producer | Dr. Natalia E. Papitashvili |
Magnetic field vector, GSE
Magnetic field vector, GSE
| Index | Name | Parameter key | Units |
|---|---|---|---|
| 1 | Bx(GSE) | Column13 | nT |
| 2 | By(GSE) | Column14 | nT |
| 3 | Bz(GSE) | Column15 | nT |
Magnetic field vector, GSM
Magnetic field vector, GSM
| Index | Name | Parameter key | Units |
|---|---|---|---|
| 1 | Bx(GSM) | Column13 | nT |
| 2 | By(GSM) | Column16 | nT |
| 3 | Bz(GSM) | Column17 | nT |
Magnetic field magnitude
Square root of sum of variances of component averages.
Standard deviation in the average of magnetic field magnitudes
Flow speed of the solar wind
Flow velocity vector, 3 GSE cartesian components
Flow velocity vector, GSE
| Index | Name | Parameter key | Units |
|---|---|---|---|
| 1 | Vx(GSE) | Column24 | km/s |
| 2 | Vy(GSE) | Column25 | km/s |
| 3 | Vz(GSE) | Column26 | km/s |
Proton density
Proton scalar temperature
Position of IMP 8 spacecraft, GSE cartesian components
Spacecraft position vector, GSE
| Index | Name | Parameter key | Units |
|---|---|---|---|
| 1 | X(IMP8,GSE) | Column29 | Re |
| 2 | Y(IMP8,GSE) | Column30 | Re |
| 3 | Z(IMP8,GSE) | Column31 | Re |
Bow shock nose position, as computed from observed data and models, 3 cartesian components
Bow shock nose (BSN) position vector, GSE
| Index | Name | Parameter key | Units |
|---|---|---|---|
| 1 | X(BSN,GSE) | Column32 | Re |
| 2 | Y(BSN,GSE) | Column33 | Re |
| 3 | Z(BSN,GSE) | Column34 | Re |
Time shift from observation time to bow shock nose (BSN) arrival time, as averaged over all 15-16 sec B values with BSN arrival times in minute of interest
Numbers of fine scale points in field and plasma averages
Numbers of fine scale points in field and plasma averages
| Index | Name | Parameter key |
|---|---|---|
| 1 | Numbers of fine scale points in field averages | Column05 |
| 2 | Numbers of fine scale points in plasma averages | Column22 |
SPASE version 2.0.0
The magnetic field experiment on the IMP-8 spacecraft utilizes a tri-axial fluxgate (saturable inductor) magnetometer. The instrument originally had three, automatically determined, ranges, ±12 nT, ±36 nT, and ±108 nT, full scale. Because of a range-change circuit failure occurring in early July 1975, the experiment was commanded into a fixed ±36 nT range on July 11, 1975 at 12:55:09 UT and has been in that range ever since. The measurements are A-to-D converted onboard, to an 8-bit resolution, yielding ±0.14 nT quantization sensitivity, which is larger than the intrinsic sensor noise level of 0.025 nT RMS. The data from the two-bit (per component) adaptive delta modulator, incorporated into the instrument, and applied to the intrinsic sample rate of 25 vectors/sec., was never utilized, and hence the rate of the full (8-bit) vector words, which occur every 320 ms, represents the effective sample period of the instrument. The sampling rate is synchronized to the spacecraft clock; the basic spacecraft clock frequency is 6.4 kHz. The sensor unit is mounted on the end of a boom approximately 4 m from the center of the spacecraft.
A web site hosting IMP-8 magnetic experiment instrument information as well as web utilities for plotting and downloading data.
Information about the Magnetic Field Experiment experiment on the IMP 8 mission.
User will acknowledge the IMP-8 magnetometer team in any publication resulting from the use of these data.
| Role | Person | |
|---|---|---|
| 1. | Principal investigator | Dr. Adam Szabo |
SPASE version 2.0.0
A modulated split-collector Faraday cup, perpendicular to the spacecraft spin axis, was used to study the directional intensity of positive ions and electrons in the solar wind, transition region, and magnetotail. The collector plate split is perpendicular to the spacecraft spin axis in order to measure the flow angle of the ions in a meridional plane; the flow angle in the spacecraft equatorial plane is determined from the fluxes measured as the spacecraft rotates.
Electrons are measured using 21 logarithmically-spaced energy windows covering the energy/charge range between 23 and 1935 volts. Positive ions are studied using 24 energy windows covering the range between 50 and 7000 volts.
The instrument has three operating modes. The tracking mode yields the best time resolution which is about 1 minute. A single energy window is used during a spacecraft rotation. The ion spectrum is obtained in eight spacecraft revolutions using a subset of the energy windows that track the peak of the solar wind. In this mode, fluxes are measured during 11.25-degree sectors of the spacecraft spin while the instrument is looking within the 90 degree sector centered on the sun direction and during 45 degree sectors for the remainder of the rotation. The other modes yield a spectrum using all 24 windows (with the same angular sectors described above) or a spectrum that results from integrating the observed fluxes over 45 degree sectors for the entire spacecraft rotation.
Electron data are obtained in all modes, but are not usually analyzed.
Parameters derived on a routine basis are proton velocity, number density, and temperature (most probable thermal speed). Those parameters are obtained from a non-linear, least-squares fit to the observed fluxes using a convected, isotropic Maxwellian model.
Key Parameters for the Plasma instrument are computed at MIT using Level Zero data that are staged to the ISTP/CDHF approximately two weeks after being received on Earth. Thus the plasma instrument's Key Parameters lag real time by something greater than 2 weeks, but less than four.
Information about the Solar Plasma Faraday Cup experiment on the IMP-J mission.
| Role | Person | |
|---|---|---|
| 1. | Principal investigator | Dr. Alan J. Lazarus |
SPASE version 2.0.0
IMP 8 (IMP-J or Explorer 50), the last satellite of the IMP series, was a drum-shaped spacecraft, 135.6 cm across and 157.4 cm high, instrumented for interplanetary and magnetotail studies of cosmic rays, energetic solar particles, plasma, and electric and magnetic fields. Its initial orbit was more elliptical than intended, with apogee and perigee distances of about 45 and 25 earth radii. Its eccentricity decreased after launch. Its orbital inclination varied between 0 deg and about 55 deg with a periodicity of several years. The spacecraft spin axis was normal to the ecliptic plane, and the spin rate was 23 rpm. The data telemetry rate was 1600 bps.
The spacecraft was in the solar wind for 7 to 8 days of every 12.5 day orbit. Telemetry coverage was 90% in the early years, but only 60-70% through most of the 1980's and early 1990's. Coverage returned to the 90% range in the mid to late 1990's.
The objectives of the extended IMP-8 operations were to provide solar wind parameters as input for magnetospheric studies and as a 1-AU baseline for deep space studies, and to continue solar cycle variation studies with a single set of well-calibrated and understood instruments.
In October, 2001, IMP 8 was terminated as an independent mission. Telemetry acquisition resumed after about three months at Canberra only (30-50% coverage), as an adjunct to the Voyager and Ulysses missions. As of August 2005 IMP 8 continued in this mode.
Information about the IMP-J mission
| Role | Person | |
|---|---|---|
| 1. | Project scientist | Dr. Robert E. McGuire |
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Space Physics Data Facility
Space Physics Data Facility
| Role | Person | |
|---|---|---|
| 1. | General contact | Ms. Tamara J. Kovalick |
| 2. | Technical contact | Mr. Robert M. Candey |
| 3. | Project scientist | Dr. Robert E. McGuire |