The CEP consisted of two identical instruments designed to measure electron
temperatures, electron and ion concentrations, ion mass, and spacecraft potential. One probe
was oriented along the spin axis of the spacecraft (normally perpendicular to the orbit plane),
and the other radially so that it could observe in the direction of the velocity vector once
each 15-s spin period. Each instrument was a retarding potential Langmuir probe device that
produced a current-voltage (I-V) curve for a known voltage pattern placed on the collector.
Electrometers were used to measure the current. There were two systems of operation (one with
two modes and another with three modes) using collector voltage patterns between plus and minus
5 volts. Most modes involved an automatic or fixed adjustment of collector voltage limits
(and/or electrometer output) such that the region of interest on the I-V profile provided
high resolution. Each system was designed for use with only one of the probes, but they
could be interswitched to provide backup redundancy. The best measurements in the most
favorable modes provided one-second time resolution; electron temperature between 300 and
1.E4 deg K (10% accuracy); ion density between 1.E4 and 1.E7 ions/cc (10-20% accuracy);
electron density between 50 and 1.E6 electrons/cc; and ion mass at ion densities above 1.E4
ions/cc. Each probe had a collector electrode extending from the central axis of a
cylindrical guard ring. The 2.5-cm-long guard ring was at the end of a 25-cm boom, and the
collector extended another 7.5 cm beyond the guard ring. The boom, guard, and collector
were 0.2 cm in diameter. More detailed information can be found in L. H. Brace et al.,
Radio Sci., v. 8, n. 4, p. 341, 1973. NSSDC has all the useful data that exist from this
investigation.
Version:2.0.0
The CEP consisted of two identical instruments designed to measure electron
temperatures, electron and ion concentrations, ion mass, and spacecraft potential. One probe
was oriented along the spin axis of the spacecraft (normally perpendicular to the orbit plane),
and the other radially so that it could observe in the direction of the velocity vector once
each 15-s spin period. Each instrument was a retarding potential Langmuir probe device that
produced a current-voltage (I-V) curve for a known voltage pattern placed on the collector.
Electrometers were used to measure the current. There were two systems of operation (one with
two modes and another with three modes) using collector voltage patterns between plus and minus
5 volts. Most modes involved an automatic or fixed adjustment of collector voltage limits
(and/or electrometer output) such that the region of interest on the I-V profile provided
high resolution. Each system was designed for use with only one of the probes, but they
could be interswitched to provide backup redundancy. The best measurements in the most
favorable modes provided one-second time resolution; electron temperature between 300 and
1.E4 deg K (10% accuracy); ion density between 1.E4 and 1.E7 ions/cc (10-20% accuracy);
electron density between 50 and 1.E6 electrons/cc; and ion mass at ion densities above 1.E4
ions/cc. Each probe had a collector electrode extending from the central axis of a
cylindrical guard ring. The 2.5-cm-long guard ring was at the end of a 25-cm boom, and the
collector extended another 7.5 cm beyond the guard ring. The boom, guard, and collector
were 0.2 cm in diameter. More detailed information can be found in L. H. Brace et al.,
Radio Sci., v. 8, n. 4, p. 341, 1973. NSSDC has all the useful data that exist from this
investigation.
Role | Person | StartDate | StopDate | Note | |
---|---|---|---|---|---|
1. | PrincipalInvestigator | spase://SMWG/Person/Larry.H.Brace |
Information about the Cylindrical Electrostatic Probes experiment on the AE-D mission.
Detailed information about the Cylindrical Electrostatic Probes on the AE-D mission.