AC6 Data

AC6 Data Download

 

 

See also AC-6 Data Browser

 

Use of this data is subject to the RULES OF THE ROAD listed below:

 

AeroCube-6 (AC6) Dosimeter Data Release
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The AC6 Dosimeter data are approved for public release. We ask that you coordinate your study with the instrument team listed below. This coordination will ensure proper considerations for data quality and avoid duplication among related studies.

 

 

The AC6 Dosimeter Team:

Bern Blake jbernard.blake@aero.org (link sends e-mail)

Drew Turner Drew.Turner@jhuapl.edu (link sends e-mail)

Paul O'Brien paul.obrien@aero.org (link sends e-mail)

 

 

 

A README file is also included:

TOR-2016-01155_AeroCube-6_Dosimeter_Data_README_v3.0.pdf - Mission and data contents description.

TOR-2017-02598 - AeroCube-6 Dosimeter Equivalent Energy Thresholds and Flux Conversion Factors.pdf - Bowtie analysis to support converting dosimeter count rates to particle fluxes.

TOR-2016-03260_-_Updated_Geant4_Simulations_of_AeroCube_6_Microdosimeters.pdf - Description of the Geant4 response simulations.


Other related files

 

 

 

 

 

The AC6 dataset is provided in 4 ASCII files each day. Survey files contain 1 Hz dosimeter data an minimal ephemeris. Coordinates file contain extended magnetic coordinates at 1 Hz. Attitude files provide detailed attitude information at 1 Hz. 10 Hz files provide the high resolution data taken in burst mode. The data dictionary indicates which quantities are in which file.

 

Column Units 1 Hz Survey 1 Hz Mag Coords 1 Hz Attitude 10 Hz Description
year   x x x x  
month   x x x x  
day   x x x x  
hour   x x x x  
minute   x x x x  
second   x x x x  
alt km x x x x Geodetic altitude
lat deg x x x x Geodetic latitude
lon deg x x x x Geodetic longitude
X_GEO RE x       X-GEO component of location
Y_GEO RE x       Y-GEO component of location
Z_GEO RE x       Z-GEO component of location
dos1l counts x     x Dos1 low output
dos1m counts x     x Dos1 medium output
dos1rate #/s x x x x Dos1 rate (>50 keV electrons, > 600 keV protons)
dos2l counts x     x Dos2 low output
dos2m counts x     x Dos2 medium output
dos2rate #/s x x x x Dos2 rate (>600 keV protons)
dos3l counts x     x Dos3 low output
dos3m counts x     x Dos3 medium output
dos3rate #/s x x x x Dos3 rate (>20 MeV protons A & B, plus >1 MeV electrons on A only)
flag   x x x x bitmap: 0 - data OK, 1 - ground contact transmitter noise, 2- crosslink transmitter noise, 4 - dubious attitude, 8 - TLE ephemeris, 16 - dos3-A noisy day
Sample_Rate Hz x       Sample rate, 1 or 10 Hz
Subcom         x Slot in multiplexed 10 Hz readout, 0 to 9
Lm_IGRF     x     McIlwain L for locally mirroring particle, IGRF magnetic field
Bmag_IGRF nT   x     Magnitude of IGRF magnetic field at vehicle
MLT_IGRF hours   x     Solar local time at equtorial crossing of IGRF magnetic field line through vehicle
InvLat_IGRF deg   x     Invariant latitude (McIlwain L) for locally mirroring particle, IGRF magnetic field
Lm_OPQ   x x   x McIlwain L for locally mirroring particle, OPQ magnetic field
Bmag_OPQ nT x x   x Magnitude of OPQ magnetic field at vehicle
MLT_OPQ hours x x   x Solar local time at equtorial crossing of OPQ magnetic field line through vehicle
InvLat_OPQ deg x x   x Invariant latitude (McIlwain L) for locally mirroring particle, OPQ magnetic field
Loss_Cone_Type   x x   x 0 - trapped, 1 - drift loss cone, 2 - bounce loss cone, -1 = open/unknown, for locally mirroring particles, OPQ magnetic field
Bx_GEO nT   x     X-GEO component of local magnetic field, OPQ model
By_GEO nT   x     Y-GEO component of local magnetic field, OPQ model
Bz_GEO nT   x     Z-GEO component of local magnetic field, OPQ model
Beq nT   x     Minimum magnetic field strength on field line through vehicle, OPQ magnetic field
I RE   x     Integral invariant for locally mirroring particle, OPQ magnetic field
K G^{1/2} RE   x     Kaufmann invariant for locally mirroring particle, OPQ magnetic field
K_Z G^{1/2} RE   x     Kaufmann invariant for normally incident particle, OPQ magnetic field
Lstar   x x     Modified third invariant (L*) for locally mirroring particle, OPQ magnetic field
Lstar_Z     x   x Modified third invariant (L*) for normally incident particle, OPQ magnetic field
hmin km x x     Minum mirror altitude around drift shell for locally mirroring particle, OPQ magnetic field
hmin_Z km   x   x Minum mirror altitude around drift shell for normally incident particle, OPQ magnetic field
Loss_Cone_Near deg   x     Polar angle of near hemisphere loss cone (100 km), OPQ magnetic field
Loss_Cone_Far deg   x     Polar angle of opposite hemisphere loss cone (100 km), OPQ magnetic field
B100N nT   x     OPQ magnetic field strength at 100 km altitude, northern hemisphere on field line through vehicle
LAT100N deg   x     Geodetic latitude at 100 km altitude, northern hemisphere, on OPQ magnetic field line through vehicle
LON100N deg   x     Geodetic longitude at 100 km altitude, northern hemisphere, on OPQ magnetic field line through vehicle
B100S nT   x     OPQ magnetic field strength at 100 km altitude, southern hemisphere on field line through vehicle
LAT100S deg   x     Geodetic latitude at 100 km altitude, southern hemisphere, on OPQ magnetic field line through vehicle
LON100S deg   x     Geodetic longitude at 100 km altitude, southern hemisphere, on OPQ magnetic field line through vehicle
Alpha deg x   x x Local pitch angle of normally incident particle, OPQ magnetic field
Alpha_X deg     x   Local pitch angle of particle moving along spacecraft X axis, OPQ magnetic field
Alpha_Y deg     x   Local pitch angle of particle moving along spacecraft Y axis, OPQ magnetic field
Alpha_Eq deg x   x   Equatorial pitch angle of normally incident particle, OPQ magnetic field
Beta deg x   x x Gyrophase angle of normally incident particle, OPQ magnetic field
Beta_X deg     x   Gyrophase angle of particle moving along spacecraft X axis, OPQ magnetic field
Beta_Y deg     x   Gyrophase angle of particle moving along spacecraft Y axis, OPQ magnetic field
Phi_B deg x   x   Longitude of OPQ magnetic field in sensor coordinates
OmegaX_GEO rad/s     x   X-GEO component of spin axis
OmegaY_GEO rad/s     x   Y-GEO component of spin axis
OmegaZ_GEO rad/s     x   Z-GEO component of spin axis
B_Spin deg     x   Angle between OPQ magnetic field and spin axis
Spin_Sun deg     x   Angle between spin axis and sun
Dist_In_Track km x     x In track distance, AC6A - AC6B
Lag_In_Track s x     x In track time separation, AC6A - AC6B
Dist_Cross_Track_Horiz km x     x Horizontal cross-track distance, AC6A - AC6B, Positive is East
Dist_Cross_Track_Vert km x     x Vertical cross-track distance, AC6A - AC6B
Dist_Total km x     x Total separation distance, AC6A - AC6B
             

 

 

 

 

 

 

 

AC6 Level 2 Data

 

 

Notice:

The form below allows to download either a selection of files, or all files in the form of a single zip file. Alternatively, you can right click on the single file, and select "Save Link As"; this allows the download of a single unzipped file

Available Data files for AC6 for 2014/




Change Year:

Select FileFile Name Spc ASelect FileFile Name Spc B
AC6-A_20141231_V03.tgz AC6-B_20141231_V03.tgz
AC6-A_20141230_V03.tgz AC6-B_20141230_V03.tgz
AC6-A_20141229_V03.tgz AC6-B_20141229_V03.tgz
AC6-A_20141221_V03.tgz AC6-B_20141221_V03.tgz
AC6-A_20141220_V03.tgz AC6-B_20141220_V03.tgz
AC6-A_20141219_V03.tgz AC6-B_20141219_V03.tgz
AC6-A_20141218_V03.tgz AC6-B_20141218_V03.tgz
AC6-A_20141217_V03.tgz AC6-B_20141213_V03.tgz
AC6-A_20141216_V03.tgz AC6-B_20141212_V03.tgz
AC6-A_20141215_V03.tgz AC6-B_20141211_V03.tgz
AC6-A_20141214_V03.tgz AC6-B_20141209_V03.tgz
AC6-A_20141213_V03.tgz AC6-B_20141208_V03.tgz
AC6-A_20141212_V03.tgz AC6-B_20141207_V03.tgz
AC6-A_20141211_V03.tgz AC6-B_20141206_V03.tgz
AC6-A_20141210_V03.tgz AC6-B_20141205_V03.tgz
AC6-A_20141209_V03.tgz AC6-B_20141204_V03.tgz
AC6-A_20141208_V03.tgz AC6-B_20141203_V03.tgz
AC6-A_20141207_V03.tgz AC6-B_20141202_V03.tgz
AC6-A_20141206_V03.tgz AC6-B_20141201_V03.tgz
AC6-A_20141205_V03.tgz AC6-B_20141130_V03.tgz
AC6-A_20141204_V03.tgz AC6-B_20141129_V03.tgz
AC6-A_20141203_V03.tgz AC6-B_20141128_V03.tgz
AC6-A_20141202_V03.tgz AC6-B_20141127_V03.tgz
AC6-A_20141201_V03.tgz AC6-B_20141126_V03.tgz
AC6-A_20141130_V03.tgz AC6-B_20141125_V03.tgz
AC6-A_20141129_V03.tgz AC6-B_20141124_V03.tgz
AC6-A_20141128_V03.tgz AC6-B_20141120_V03.tgz
AC6-A_20141127_V03.tgz AC6-B_20141117_V03.tgz
AC6-A_20141126_V03.tgz AC6-B_20141116_V03.tgz
AC6-A_20141125_V03.tgz AC6-B_20141115_V03.tgz
AC6-A_20141124_V03.tgz AC6-B_20141114_V03.tgz
AC6-A_20141123_V03.tgz AC6-B_20141113_V03.tgz
AC6-A_20141122_V03.tgz AC6-B_20141112_V03.tgz
AC6-A_20141121_V03.tgz AC6-B_20141111_V03.tgz
AC6-A_20141120_V03.tgz AC6-B_20141110_V03.tgz
AC6-A_20141119_V03.tgz AC6-B_20141109_V03.tgz
AC6-A_20141118_V03.tgz AC6-B_20141108_V03.tgz
AC6-A_20141117_V03.tgz AC6-B_20141107_V03.tgz
AC6-A_20141116_V03.tgz AC6-B_20141106_V03.tgz
AC6-A_20141115_V03.tgz AC6-B_20141105_V03.tgz
AC6-A_20141114_V03.tgz AC6-B_20141104_V03.tgz
AC6-A_20141113_V03.tgz AC6-B_20141103_V03.tgz
AC6-A_20141112_V03.tgz AC6-B_20141102_V03.tgz
AC6-A_20141111_V03.tgz AC6-B_20141101_V03.tgz
AC6-A_20141110_V03.tgz AC6-B_20141031_V03.tgz
AC6-A_20141109_V03.tgz AC6-B_20141030_V03.tgz
AC6-A_20141108_V03.tgz AC6-B_20141029_V03.tgz
AC6-A_20141107_V03.tgz AC6-B_20141028_V03.tgz
AC6-A_20141106_V03.tgz AC6-B_20141027_V03.tgz
AC6-A_20141105_V03.tgz AC6-B_20141026_V03.tgz
AC6-A_20141104_V03.tgz AC6-B_20141025_V03.tgz
AC6-A_20141103_V03.tgz AC6-B_20141024_V03.tgz
AC6-A_20141102_V03.tgz AC6-B_20141023_V03.tgz
AC6-A_20141101_V03.tgz AC6-B_20141022_V03.tgz
AC6-A_20141031_V03.tgz AC6-B_20141021_V03.tgz
AC6-A_20141030_V03.tgz AC6-B_20141020_V03.tgz
AC6-A_20141029_V03.tgz AC6-B_20141019_V03.tgz
AC6-A_20141028_V03.tgz AC6-B_20141018_V03.tgz
AC6-A_20141027_V03.tgz AC6-B_20141017_V03.tgz
AC6-A_20141026_V03.tgz AC6-B_20141016_V03.tgz
AC6-A_20141025_V03.tgz AC6-B_20141015_V03.tgz
AC6-A_20141024_V03.tgz AC6-B_20141014_V03.tgz
AC6-A_20141023_V03.tgz AC6-B_20141013_V03.tgz
AC6-A_20141022_V03.tgz AC6-B_20141012_V03.tgz
AC6-A_20141021_V03.tgz AC6-B_20141011_V03.tgz
AC6-A_20141020_V03.tgz AC6-B_20141010_V03.tgz
AC6-A_20141019_V03.tgz AC6-B_20141009_V03.tgz
AC6-A_20141018_V03.tgz AC6-B_20141008_V03.tgz
AC6-A_20141017_V03.tgz AC6-B_20141007_V03.tgz
AC6-A_20141016_V03.tgz AC6-B_20141003_V03.tgz
AC6-A_20141015_V03.tgz AC6-B_20141002_V03.tgz
AC6-A_20141014_V03.tgz AC6-B_20141001_V03.tgz
AC6-A_20141013_V03.tgz AC6-B_20140930_V03.tgz
AC6-A_20141012_V03.tgz AC6-B_20140929_V03.tgz
AC6-A_20141011_V03.tgz AC6-B_20140928_V03.tgz
AC6-A_20141010_V03.tgz AC6-B_20140927_V03.tgz
AC6-A_20141009_V03.tgz AC6-B_20140926_V03.tgz
AC6-A_20141008_V03.tgz AC6-B_20140925_V03.tgz
AC6-A_20141007_V03.tgz AC6-B_20140924_V03.tgz
AC6-A_20141006_V03.tgz AC6-B_20140923_V03.tgz
AC6-A_20141005_V03.tgz AC6-B_20140922_V03.tgz
AC6-A_20141004_V03.tgz AC6-B_20140921_V03.tgz
AC6-A_20141003_V03.tgz AC6-B_20140920_V03.tgz
AC6-A_20141002_V03.tgz AC6-B_20140916_V03.tgz
AC6-A_20141001_V03.tgz AC6-B_20140915_V03.tgz
AC6-A_20140930_V03.tgz AC6-B_20140914_V03.tgz
AC6-A_20140929_V03.tgz AC6-B_20140913_V03.tgz
AC6-A_20140928_V03.tgz AC6-B_20140912_V03.tgz
AC6-A_20140927_V03.tgz AC6-B_20140911_V03.tgz
AC6-A_20140926_V03.tgz AC6-B_20140910_V03.tgz
AC6-A_20140925_V03.tgz AC6-B_20140909_V03.tgz
AC6-A_20140924_V03.tgz AC6-B_20140908_V03.tgz
AC6-A_20140923_V03.tgz AC6-B_20140905_V03.tgz
AC6-A_20140922_V03.tgz AC6-B_20140904_V03.tgz
AC6-A_20140921_V03.tgz AC6-B_20140903_V03.tgz
AC6-A_20140920_V03.tgz AC6-B_20140902_V03.tgz
AC6-A_20140919_V03.tgz AC6-B_20140901_V03.tgz
AC6-A_20140917_V03.tgz AC6-B_20140831_V03.tgz
AC6-A_20140916_V03.tgz AC6-B_20140829_V03.tgz
AC6-A_20140912_V03.tgz AC6-B_20140828_V03.tgz
AC6-A_20140911_V03.tgz AC6-B_20140827_V03.tgz
AC6-A_20140910_V03.tgz AC6-B_20140825_V03.tgz
AC6-A_20140909_V03.tgz AC6-B_20140824_V03.tgz
AC6-A_20140908_V03.tgz AC6-B_20140823_V03.tgz
AC6-A_20140906_V03.tgz AC6-B_20140822_V03.tgz
AC6-A_20140905_V03.tgz AC6-B_20140821_V03.tgz
AC6-A_20140904_V03.tgz AC6-B_20140820_V03.tgz
AC6-A_20140903_V03.tgz AC6-B_20140819_V03.tgz
AC6-A_20140902_V03.tgz AC6-B_20140818_V03.tgz
AC6-A_20140901_V03.tgz AC6-B_20140817_V03.tgz
AC6-A_20140831_V03.tgz AC6-B_20140816_V03.tgz
AC6-A_20140829_V03.tgz AC6-B_20140725_V03.tgz
AC6-A_20140828_V03.tgz AC6-B_20140724_V03.tgz
AC6-A_20140827_V03.tgz AC6-B_20140722_V03.tgz
AC6-A_20140826_V03.tgz AC6-B_20140721_V03.tgz
AC6-A_20140825_V03.tgz AC6-B_20140719_V03.tgz
AC6-A_20140824_V03.tgz AC6-B_20140718_V03.tgz
AC6-A_20140823_V03.tgz AC6-B_20140717_V03.tgz
AC6-A_20140822_V03.tgz AC6-B_20140716_V03.tgz
AC6-A_20140821_V03.tgz AC6-B_20140715_V03.tgz
AC6-A_20140820_V03.tgz AC6-B_20140714_V03.tgz
AC6-A_20140819_V03.tgz AC6-B_20140710_V03.tgz
AC6-A_20140818_V03.tgz AC6-B_20140628_V03.tgz
AC6-A_20140817_V03.tgz AC6-B_20140626_V03.tgz
AC6-A_20140816_V03.tgz AC6-B_20140621_V03.tgz
AC6-A_20140809_V03.tgz
AC6-A_20140808_V03.tgz
AC6-A_20140807_V03.tgz
AC6-A_20140806_V03.tgz
AC6-A_20140805_V03.tgz
AC6-A_20140804_V03.tgz
AC6-A_20140802_V03.tgz
AC6-A_20140801_V03.tgz
AC6-A_20140731_V03.tgz
AC6-A_20140725_V03.tgz
AC6-A_20140724_V03.tgz
AC6-A_20140723_V03.tgz
AC6-A_20140722_V03.tgz
AC6-A_20140721_V03.tgz
AC6-A_20140719_V03.tgz
AC6-A_20140718_V03.tgz
AC6-A_20140717_V03.tgz
AC6-A_20140716_V03.tgz
AC6-A_20140715_V03.tgz
AC6-A_20140714_V03.tgz
AC6-A_20140711_V03.tgz
AC6-A_20140710_V03.tgz
AC6-A_20140709_V03.tgz
AC6-A_20140628_V03.tgz
AC6-A_20140626_V03.tgz
AC6-A_20140621_V03.tgz