************************************ AE-D ************************* ************* BRIEF DESCRIPTIONS OF THE SATELLITE AND EXPERIMENTS ** ************************************ AE-D ************************** Spacecraft Common Name- AE-D NSSDC ID- 75-096A Launch Date- 10/06/75 Weight- 681. KG Orbit Parmeters Orbit Type- Geocentric Epoch Date- 1975-10-07 Orbit Period- 126.9 min Inclination- 90.1 DEG Periapsis- 154. KM_ALT Apoapsis- 3816. KM_ALT The purpose of the AE-D mission was to continue the investigation begun by AE-C of the chemical processes and energy transfer mechanisms that control the structure and behavior of the earth's atmosphere and ionosphere in the region of high absorption of solar energy. This mission was planned to sample the high latitude regions at the same time that the AE-E mission was sampling the equatorial and low latitude regions. The same type of spacecraft as AE-C was used, and the payload consisted of the same types of instruments except for deletion of the extreme solar UV monitor and the Bennett ion mass spectrometer, which were part of the AE-E payload. The polar orbit provided the sampling of all latitudes and the perigee moved through all latitudes in 3 months and all local times in 4 months. Unfortunately, a failure in the power supply system resulted in the termination of operations on January 29, 1976, after slightly less than 4 months of useful life. However, all the regions at the perigee altitudes were sampled during this time. The spacecraft re-entered the atmosphere about 1 month after cessation of telemetry. A nutation problem prevented the acquistion of temperature data and required a more extensive data reduction than for the other satellites. To continue the correlated observations with the AE-E mission, AE-C was reactivated on February 28, 1976, to replace AE-D. More details about the spacecraft and mission can be found in A. Dalgarno et al., Radio Sci., v. 8, n. 4, p. 263, 1973. --------------------------------- AE-D,BRACE ----------------------------------- Investigation Name- Cylindrical Electrostatic Probe (CEP) NSSDC ID- 75-096A-01 Personnel OI - R.F. THEIS NASA-GSFC OI - A. DALGARNO SAO PI - L.H. BRACE NASA-GSFC Brief Description 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. -------------------------------- AE-D,CHAMPION --------------------------------- Investigation Name- Atmospheric Density Accelerometer (MESA) NSSDC ID- 75-096A-02 Personnel OI - F.A. MARCOS USAF GEOPHYS LAB PI - K.S. CHAMPION USAF GEOPHYS LAB Brief Description The Miniature Electrostatic Analyzer (MESA) obtained data on the neutral density of the atmosphere in the altitude range of 120 to 400 km by the measurements of satellite deceleration due to aerodynamic drag. The instrument consisted of three single-axis accelerometers, mounted mutually at right angles, two in the spacecraft X-Y plane and the other in the Z-axis. The instrument determined the applied acceleration from the electrostatic force required to recenter a proof mass. The output of the device was a digital pulse rate proportional to the applied acceleration. The sample time of each measurement was 0.25 s. The measurements allowed determination of the density of the neutral atmosphere, monitored the thrust of the orbit-adjust propulsion system (OAPS), determined the satellite minimum altitude, measured spacecraft roll, and provided some attitude-sensing information. Spacecraft nutations of less than 0.01 deg were monitored. The instrument had three sensitivity ranges: 8.E-3 earth's gravity (G) in OAPS monitor mode; 4.E-4 G between 120 km (plus or minus 2%) and 280 km (plus or minus 10%); and 2.E-5 G between 180 km (plus or minus 2%) and 400 km (plus or minus 10%). Numbers in parentheses represent errors. A systematic error of up to plus or minus 5% due to drag coefficient uncertainty was also possible. The highest measurement altitude was determined assuming the instrument could sense to 0.2% of full scale. More details can be found in K. S. W. Champion et al., Radio Sci., v. 8, n. 4, p. 297, 1973. NSSDC has all the data that exist from this investigation. -------------------------------- AE-D,DOERING ---------------------------------- Investigation Name- Photoelectron Spectrometer (PES) NSSDC ID- 75-096A-03 Personnel OI - J.C. ARMSTRONG APPLIED PHYSICS LAB OI - C.O. BOSTROM APPLIED PHYSICS LAB PI - J.P. DOERING JOHNS HOPKINS U Brief Description This experiment was designed to provide information on the intensity, angular distribution, energy spectrum, and net flows along field lines, of electrons in the thermosphere with energies between 1 and 500 eV. The instrument consisted of two identical oppositely directed hemispherical electrostatic analyzers, and it had 30 operating modes. Each spectrometer had a relative energy resolution plus or minus 2.5% and a geometric factor on the order of 0.001 sq cm sr, independent of electron energy. Three separate energy ranges could be sensed: 0 to 25, 0 to 100, or 0 to 500 eV. Measurements from these intervals could be sequenced in 5 different ways. Data could be taken from either sensor separately, or alternately with time resolution varying from 0.25 to 8 s. There were two deflection voltage scan rates determined by spacecraft clock. This voltage was changed in 64 steps, and was done at 4 or 16 steps per telemetry frame. With 16 frames/s, this allowed a choice of either one 64-point spectrum, or four 16-point spectra in 1 s. The longest (8 s) cycle of data involved observations using increasing voltage steps for the lowest, middle, lowest, then highest energy ranges (in that order) for 1 s each. A repeat for decreasing voltage steps completed the cycle. A more detailed description of this experiment may be found in J. P. Doering et al., Radio Sci., v. 8, n. 4, p. 387, 1973. NSSDC has all the useful data that exist from this investigation. --------------------------------- AE-D,HANSON ---------------------------------- Investigation Name- Retarding Potential Analyzer/Drift Meter NSSDC ID- 75-096A-04 Personnel OI - S. SANATANI U OF TEXAS, DALLAS OI - D.R. ZUCCARO U OF TEXAS, DALLAS OI - C.R. LIPPENCOTT U OF TEXAS, DALLAS PI - W.B. HANSON U OF TEXAS, DALLAS Brief 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 heads were spaced almost 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 purpose 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 4-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. ------------------------------ AE-D,HINTEREGGER -------------------------------- Investigation Name- Solar EUV Spectrophotometer (EUVS) NSSDC ID- 75-096A-06 Personnel OI - C.W. CHAGNON USAF GEOPHYS LAB OI - D.E. BEDO USAF GEOPHYS LAB OI - L.A. HALL USAF GEOPHYS LAB OI - J.E. MANSON USAF GEOPHYS LAB PI - H.E. HINTEREGGER USAF GEOPHYS LAB Brief Description The Extreme Ultraviolet Spectrometer (EUVS) was used to observe the variations in the solar EUV flux in the wavelength range from 140 to 1850 A and the atmospheric attenuation at various fixed wavelengths. This provided quantitative atmospheric structure and composition data. The instrument consisted of 24 grazing-incidence grating monochromators, using parallel-slit systems for entrance collimation and photoelectric detectors at the exit slits. Twelve of these monochromators had wavelength scan capability, each with 128 selectable wavelength positions, which could also automatically step scan through these positions. The other 12 monochromators operated at fixed wavelengths with fields of view smaller than the full solar disk to aid in the atmospheric absorption analysis. The spectral resolution varied from 2 to 54 A depending upon the particular instrument. The field of view varied from 60 x 60 arc min down to 3 x 6 arc min. All 24 monochromator-entrance axes were co-aligned parallel. A solar point system could point to 256 different positions, execute a 16-step one-dimensional scan or a full 256-step raster. The time resolution varied from 0.5 s for observing 12 fixed wavelengths up to 256 s for programming the EUVS through all possible modes. More details can be found in H. E. Hinteregger et al., Radio Sci., v. 8, n. 4, p. 349, 1973. ---------------------------------- AE-D,NIER ----------------------------------- Investigation Name- Open-Source Neutral Mass Spectrometer NSSDC ID- 75-096A-07 Personnel OI - W.E. POTTER U OF MINNESOTA OI - K. MAUERSBERGER U OF MINNESOTA PI - A.O. NIER U OF MINNESOTA Brief Description The objective of this experiment was to contribute to a study of the chemical, dynamic, and energetic processes that control the structure of the thermosphere by providing direct, in situ measurements of both major and minor neutral atmospheric constituents having masses in the range from 1 to 48 atomic mass units (u). A double-focusing Mattauch-Herzog magnetic deflection mass spectrometer with an impact ion source was flown. Two ion collectors were included to measure ions differing in mass by a factor of 8, i.e., the two mass ranges covered were 1 to 6 u and 6 to 48 u. In the ion source the neutral species were ionized by means of electron impact. At altitudes greater than 380 km, ion currents were measured with an electron multiplier counting individual ions. Counts were accumulated for 1/20 s before automatically switching to a different mass number. While complete mass spectra could be swept, in the common mode of operation peak stepping was employed, with readings on the principal peaks in the mass spectrum being repeated approximately every 0.5 s and on other species less frequently. Data below 380 km were measured using an electrometer. In addition to the peak-stepping mode, there were several other operating modes which were selected by ground command. In the fly-through mode, the ion source voltages were adjusted so that there was no electric field to draw ions out of the electron beam when they were formed. Ambient particles striking the ion source retained energies less than 0.1 eV, which is not high enough to overcome the negative space charge potential holding the ions in the beam. Those ambient particles that did not strike the ion source retained their incoming energy of several eV after ionization and escaped into the accelerating region of the analyzer. The electron accelerating potential was 75 eV in normal mode operation and 25 eV in the fly-through mode. In another operating mode, the instrument switched automatically to a sequence of masses of particular interest such as, e.g., between masses 16 and 32 or between masses 28 and 32. More experiment details can be found in A. O. Nier et al., Radio Sci., v. 8, n. 4, p. 271, 1973. NSSDC has all the useful data that exist from this investigation. --------------------------------- AE-D,HEDIN ----------------------------------- Investigation Name- Neutral Atmosphere Composition (NACE) NSSDC ID- 75-096A-08 Personnel OI - G.R. CARIGNAN U OF MICHIGAN OI - C.A. REBER NASA-GSFC PI - A.E. HEDIN NASA-GSFC Brief Description This experiment measured in situ the spatial distribution and temporal changes of the concentrations of the neutral atmospheric species. In addition, new insight into in situ measurement techniques was obtained from comparisons of these measurements with other onboard experiments: namely, open-source spectrometer (75-096A-07), solar EUV spectrophotometer (75-096A-06), and density accelerometer (75-096A-02). The mass-spectrometer sensor included a gold-plated stainless steel thermalizing chamber and ion source, a hyperbolic-rod quadrupole analyzer, and an off-axis electron multiplier. Five different sequences of mass selection were available and, expressed in atomic mass units (u), were as follows: (1) geophysical -1, 2, 4, total, 16, 28, 32, selected, 40, (2) analytical -12, 14, 18, 20, 22, 30, 44, calibrate, zero, (3) individual -selected, selected, selected, ... (any mass 1 to 44), (4) sweep digital -1, 2, 3, 4, 5, ... 45 (in 3/16-u steps), (5) sweep analog 2, 3, 4, 5, ... 45 (continuous). Five operational formats were available and selected by ground command. When operating in the "normal" format, the analyzer measured all masses in the range 1 to 44 with emphasis on hydrogen, helium, oxygen, nitrogen, and argon. Another format was optimized for minor constituent studies of any individual gas species in the measured range. Spatial resolution was determined primarily by the mode of spacecraft operation. In orbit, the presealed spectrometer was opened, and the atmospheric constituents passed through a knife-edged orifice into the thermalization chamber and ion source. Selected ions left the quadrupole analyzer through a weak focusing lens and were accelerated into a 14-stage electron multiplier, where they were turned 90 deg to strike the first dynode. For each impacting ion, the multiplier output was a pulse of 2.E6 electrons. These output pulses constituted the measurement and the count rate was proportional to the chamber density of the selected species. These density values were converted to ambient concentrations. The analyzer normally operated at a resolution of 1 u over the mass range, so that a mass peak one-thousandth the amplitude of an adjacent peak could be measured. For the dynamic range required, pulses occurring during 0.015-s integration intervals were accumulated in a 16-bit counter. Multiple integration periods (up to 16) were assigned to each measurement for less dense atmospheric species. Automatically selected ranges of ionizing electron currents were used. The overall range of the measurements was planned to be greater than 1.E7. There was a provision for the instrument orifice to be covered during spacecraft thruster operations. More experiment details can be found in D. T. Pelz et al., Radio Sci., v. 8, n. 4, p. 277, 1973. NSSDC has all the useful data that exist from this investigation. -------------------------------- AE-D,SPENCER ---------------------------------- Investigation Name- Neutral Atmosphere Temperature (NATE) NSSDC ID- 75-096A-09 Personnel OI - G.R. CARIGNAN U OF MICHIGAN OI - H.B. NIEMANN NASA-GSFC PI - N.W. SPENCER NASA-GSFC Brief Description This experiment was designed to measure the kinetic temperature of the neutral atmosphere by determining the instantaneous density of molecular nitrogen in a spherical chamber coupled to the atmosphere through a knife-edge orifice. Analysis of the measured molecular nitrogen density variation over a spin cycle with a knowledge of the satellite's motion and orientation led to a determination of the ambient temperature, independent of scale height. The NATE also provided measurements of the neutral composition, when commanded into the appropriate mode. In addition, values for the zonal wind were obtained, from measurement of the "stream" position relative to the satellite velocity. An alternate measurement of neutral temperature also was undertaken, using a baffle inserted in front of the orifice to intercept a portion of the gas particle stream entering the chamber. When the satellite was in the despun mode, the baffle was made to oscillate in the stepwise fashion in order to interrupt the particle stream seen by the orificed chamber. These chamber density variations were interpreted to yield the neutral gas kinetic temperature also. A dual-filament ion source sampled the thermalized molecular nitrogen in the chamber and produced an ion beam density proportional to the nitrogen chamber density. From the source, the ionized beam was directed to a quadrupole analyzer, tuned to pass those particles whose mass-to-charge ratio (M/Q) was 28. This ionized nitrogen beam then passed on to an electron multiplier. The output pulses were amplified and counted in a 16-bit accumulator. The sensor was vacuum-sealed prior to launch and opened to the atmosphere after the spacecraft was in orbit. More experiment details can be found in N. W. Spencer et al., Radio Sci., v. 8, n. 4, p. 287, 1973. NSSDC has all the useful data that exist from this investigation. -------------------------------- AE-D,HOFFMAN ---------------------------------- Investigation Name- Magnetic Ion-Mass Spectrometer (MIMS) NSSDC ID- 75-096A-10 Personnel OI - W.B. HANSON U OF TEXAS, DALLAS OI - C.R. LIPPENCOTT U OF TEXAS, DALLAS OI - E.E. FERGUSON NOAA-ERL PI - J.H. HOFFMAN U OF TEXAS, DALLAS Brief Description A magnetic ion-mass spectrometer was flown to measure in situ the concentrations of the ambient positive ion species in the mass range from 1 to 90 atomic mass units (u). Mounted on the satellite equator normal to the spin axis, the entrance aperture faced forward when the spacecraft was in the despun mode. The electric and magnetic fields were arranged to produce a mass spectrum along the focal plane following the magnetic analyzer. Three slits were placed along this plane in appropriate places to simultaneously collect ions in the mass ratio 1-4-16. Ionospheric ions were accelerated into the analyzer system by a negative voltage that varied from -1060 to -225 V. The three mass ranges measured simultaneously were 1 to 4, 4 to 16, and 14 to 72 u. Following each slit was an electron multiplier and logarithmic electrometer-amplifier detector. The detector output was either measured directly for an analog output, or was supplied to a "peak" circuit that determined the amplitude of each peak in the spectrum. Only the amplitude of each peak was telemetered in the "peak" mode, and in this mode the time required to simultaneously sweep all three mass ranges was 1 s. Other modes of operation were possible. In the analog short mode, the three mass ranges were swept in 2 s, alternating with 1-s "peak" mode scans. An 8-s sweep time was required in the analog long mode, again alternating with 1-s "peak" mode scans. An option existed in the locked mode to continuously measure any set of mass numbers in the ratio 1-4-16 to give high spatial resolution. More experiment detail can be found in J. H. Hoffman et al., Radio Sci., v. 8, n. 4, p. 315, 1973. NSSDC has all the useful data that exist from this investigation. --------------------------------- AE-D,BARTH ----------------------------------- Investigation Name- Ultraviolet Nitric-Oxide Experiment NSSDC ID- 75-096A-11 Personnel OI - D.W. RUSCH U OF COLORADO OI - A.I. STEWART U OF COLORADO PI - C.A. BARTH U OF COLORADO Brief Description This Ultraviolet Nitric-Oxide Experiment (UVNO) consisted of a two-channel fixed-grating Ebert-Fastie spectrometer, which measured the airglow in the (1, 0) Gamma band in a 15-A region centered at 2149 A. The observed intensity was produced by resonance fluorescence of sunlight by the nitric-oxide molecules in the instrument's field of view. The intensity data obtained yielded altitude profiles of nitric-oxide density as a function of time and location. The remote sensing character of the UVNO experiment permitted measurements of nitric-oxide to be made at altitudes both above and below satellite perigee. As the spacecraft spun, the spectrometer, which looked outward through the rim of the satellite, repeatedly had its field of view carried down through the atmosphere onto the earth's limb, and altitude profiles of the emitted airglow intensity were obtained. Below some altitude the measured signal at 2149 A was contaminated by rayleigh-scattered sunlight. To correct for this contamination, a second channel measured only scattered light intensity in a 12-A region centered at 2190 A. The two channels were optically and electrically independent. Nitric-oxide airglow intensity was determined by taking the difference between these two measurements. The sensor's spherical fused-quartz telescope mirror had a 125-mm focal length, and focused incident light on the entrance slit of the spectrometer. From this slit the light struck one-half of the mirror and was collimated onto the grating. The 3600-lines-per-mm grating returned the light collimated to the other half of the mirror, and the light was focused on two exit slits. The spectrometer field of view was 4 deg X 1/4 deg, with the long axis parallel to the spacecraft's spin axis, and therefore parallel to the viewed limb. In normal operation each channel was integrated for 20.8 ms and read out alternately at 10.4-ms intervals. The instrument was protected against contamination from internal scattering of off-axis undispersed light. More experiment details can be found in C. A. Barth et al., Radio Sci., v. 8, n. 4, p. 379, 1973. NSSDC has all the useful data that exist from this investigation. -------------------------------- AE-D,HOFFMAN ---------------------------------- Investigation Name- Low-Energy Electrons (LEE) NSSDC ID- 75-096A-12 Personnel OI - D.S. EVANS NOAA-ERL OI - J.L. BURCH SOUTHWEST RES INST PI - R.A. HOFFMAN NASA-GSFC Brief Description This experiment furnished direct measurements of the energy input into the upper atmosphere due to electrons and protons (ions) in the energy range 0.2 to 25 keV. The fluxes of electrons and ions were measured with cylindrical electrostatic analyzers and Spiraltron electron multipliers. There were 19 detectors, one ion stepped-energy analyzer, and two electron stepped analyzers mounted at different angles. In addition, there were 16 fixed energy detectors which obtained high-time-resolution angular distributions, in the spacecraft one revolution-per-orbit mode, at five energies between 0.72 and 18 keV. More details can be found in R. A. Hoffman et al., Radio Sci., v. 8, n. 4, p. 393, 1973. NSSDC has all the useful data that exist from this investigation. ---------------------------------- AE-D,HAYS ----------------------------------- Investigation Name- Visible Airglow Photometer (VAE) NSSDC ID- 75-096A-13 Personnel OI - G.R. CARIGNAN U OF MICHIGAN OI - G.G. SHEPHERD YORK U OI - J.C. WALKER U OF MICHIGAN PI - P.B. HAYS U OF MICHIGAN Brief Description The visible airglow experiment provided volume emission rates for several dayglow, nightglow, and auroral optical emission features. A photometer containing two separate optical channels was used. Spectral selection was accomplished with a common filter wheel that contained six interference filters and a dark and calibrate position. The wavelengths measured in pairs (in Angstroms) were 7319 and 4861, 5200 and dark, 5577 and 7319, 4278 and 5200, 6300 and 5577, calibration and 4278, and 4861 and 6300. The two channels were separated in angle by 90 deg. One channel had a large field of view (3 deg half-angle) for high sensitivity, normally pointing toward the local zenith, and the second channel had a small field of view (0.75 deg half-angle) for high spatial resolution, pointing tangent to the surface of the earth when the satellite was in the despun mode. Both channels were protected from stray light contamination during daytime by multistage baffle systems. Photons that had been spectrally and spatially selected were sensed by a pulse-counting photomultiplier system capable of counting at a rate of 5.E6 counts/s. The filters could be operated in several modes, e.g., fixed filter, and automatic filter changes could be synchronized either to satellite orientation or to a fixed-time base. More experiment details can be found in P. B. Hays et al., Radio Sci., v. 8, n. 4, p. 369, 1973. NSSDC has all the useful data that exist from this investigation.