Especially in the second section, users will see quantities
present which may then disappear, and later come back. Status
cycling and testing were happening during this section. It was
felt that extensive editing of the NSSDC submission to include
only data being measured for only the times it was measured would
have been both time consuming and confusing. Instead we have provided
general indications of when this is happening. Users needing more
detailed data on instrument performance are urged to contact
Dr. Nand Lal
(301) 286-7350.
The following is a description of our mnemonic naming convention for the potential fluxes and rates present in our database if all data quantities were present for the cruise lifetime. To see a list of the exact data quantities we have included in the archive data files for each of the three periods described above, click on the representative time. The data files are segmented into yearly datasets, except for 1979 and 1982, where our time period breaks occur.
Launch - 06/29/79
08/22/79 - 04/22/82
04/22/82 - 12/31/92
The phrases 2 dimensional analysis or 3 dimensional analysis in the following description refer to events whose analysis utilized pulse height data from either 2 or 3 pulse height values associated with the particular event type (detector element coincidence requirement) being measured at the time.
As an example, for A side events, particles enter the HET telescope from the A end, and
----------------------------------
HET fluxes :
----------------------------------
HELIUMFLUX1 Helium4 flux in particles/cm**2.s.sr.Mev/n
A-stopping 2 dimensional analysis, high
gain data from HET-I
4.2 - 6.0 MeV/nucleon energy range
----------------------------------
HELIUMFLUX2 Helium4 flux as above, A-stopping,
3 dimensional analysis, high gain data
from HET-I
6.0 - 42.0 MeV/n energy range,
----------------------------------
HELIUMFLUX3 B-stopping 2 dimensional analysis, low
gain HET-I
17.0 - 27.0 MeV/n
----------------------------------
HELIUMFLUX4 B-stopping 3 dimensional analysis, low
gain HET-I
30.0 - 69.0 MeV/n
----------------------------------
HELIUMFLUX5 B-stopping 2 dimensional analysis, high
gain HET-I
17.0 - 27.0 MeV/n
----------------------------------
HELIUMFLUX6 B-stopping 3 dimensional analysis, high
gain data from HET-I
30.0 - 69.0 MeV/n
----------------------------------
HELIUMFLUX7 B-penetrating 3 dimensional analysis, low
gain penetrating data from HET-I
193.125 - 480.5 MeV/n
----------------------------------
HELIUMFLUX8 B-penetrating 3 dimensional analysis, high
gain penetrating data from HET-I
191.925 - 475.7 MeV/n energy range
----------------------------------
PROTONFLUX1 Proton flux in particles/cm**2.s.sr.MeV/n
A-stopping 2 dimensional analysis, high
gain data from HET-I
4.2 - 6.0 MeV energy range
----------------------------------
PROTONFLUX2 Proton flux in particles/cm**2.s.sr.MeV/n
3 dimensional analysis, high gain data from
HET-I
6.0 - 42.0 MeV energy range,
----------------------------------
PROTONFLUX3 B-stopping 2 dimensional analysis, high
gain data from HET-I
17.0 - 27.0 MeV energy range
----------------------------------
PROTONFLUX4 B-stopping 3 dimensional analysis, high
gain data from HET-I
30.0 - 69.0 MeV energy range
----------------------------------
PROTONFLUX5 B-penetrating 3 dimensional analysis, high
gain penetrating data from HET-I
132.834 - 241.963 MeV energy range
----------------------------------
HELIUMFLUX9 Helium4 flux in particles/cm**2.s.sr.Mev/n
A-stopping 2 dimensional analysis, high
gain data from HET-II
4.2 - 6.0 MeV/n energy range
----------------------------------
HELIUMFLUX10 Helium4 flux as above, A-stopping,
3 dimensional analysis, high gain data
from HET-II
6.0 - 42.0 MeV/n energy range,
----------------------------------
HELIUMFLUX11 B-stopping 2 dimensional analysis, low
gain HET-II
17.0 - 27.0 MeV/n
----------------------------------
HELIUMFLUX12 B-stopping 3 dimensional analysis, low
gain HET-II
30.0 - 69.0 MeV/n
----------------------------------
HELIUMFLUX13 B-stopping 2 dimensional analysis, high
gain HET-II
17.0 - 27.0 MeV/n
HELIUMFLUX14 B-stopping 3 dimensional analysis, high
gain data from HET-II
30.0 - 69.0 MeV/n
----------------------------------
HELIUMFLUX15 B-penetrating 3 dimensional analysis, low
gain penetrating data from HET-II
193.125 - 480.486 MeV/n
----------------------------------
HELIUMFLUX16 B-penetrating 3 dimensional analysis, high
gain penetrating data from HET-II
191.925 - 475.705 MeV/n energy range
----------------------------------
PROTONFLUX6 Proton flux in particles/cm**2.s.sr.MeV/n
A-stopping 2 dimensional analysis, high
gain data from HET-II
4.2 - 6.0 MeV energy range
----------------------------------
PROTONFLUX7 Proton flux in particles/cm**2.s.sr.MeV/n
3 dimensional analysis, high gain data from
HET-II
6.0 - 42.0 MeV energy range,
----------------------------------
PROTONFLUX8 B-stopping 2 dimensional analysis, high
gain data from HET-II
17.0 - 27.0 MeV energy range
----------------------------------
PROTONFLUX9 B-stopping 3 dimensional analysis, high
gain data from HET-II
30.0 - 69.0 MeV energy range
----------------------------------
PROTONFLUX10 B-penetrating 3 dimensional analysis, high
gain penetrating data from HET-II
132.834 - 241.963 MeV energy range
----------------------------------
----------------------------------
LET fluxes : (all stopping particle events)
----------------------------------
PROTONFLUX11 Proton 2-dimensional analysis from LET-A
energy range of 1.8 - 3.3 MeV
----------------------------------
PROTONFLUX12 Proton 2-dimensional analysis from LET-B
energy range of 1.8 - 3.3 MeV
----------------------------------
PROTONFLUX13 Proton 2-dimensional analysis from LET-C
energy range of 1.8 - 3.3 MeV
----------------------------------
PROTONFLUX14 Proton 2-dimensional analysis from LET-D
energy range of 1.8 - 3.3 MeV
----------------------------------
PROTONFLUX15 Proton 3-dimensional analysis from LET-A
energy range of 3.25 - 8.1 MeV
----------------------------------
PROTONFLUX16 Proton 3-dimensional analysis from LET-B
energy range of 3.25 - 8.1 MeV
----------------------------------
PROTONFLUX17 Proton 3-dimensional analysis from LET-C
energy range of 3.25 - 8.1 MeV
----------------------------------
PROTONFLUX18 Proton 3-dimensional analysis from LET-D
energy range of 3.25 - 8.1 MeV
----------------------------------
----------------------------------
HELIUMFLUX17 Helium4 2-dimensional analysis from LET-A
1.800 - 2.800 MeV/n energy range
----------------------------------
HELIUMFLUX18 Helium4 2-dimensional analysis from LET-B
1.800 - 2.800 MeV/n energy range
----------------------------------
HELIUMFLUX19 Helium4 2-dimensional analysis from LET-C
1.800 - 2.800 MeV/n energy range
----------------------------------
HELIUMFLUX20 Helium4 2-dimensional analysis from LET-D
1.800 - 2.800 MeV/n energy range
----------------------------------
HELIUMFLUX21 Helium4 3-dimensional analysis from LET-A
2.800 - 8.000 MeV/n energy range
----------------------------------
HELIUMFLUX22 Helium4 3-dimensional analysis from LET-B
2.800 - 8.000 MeV/n energy range
----------------------------------
HELIUMFLUX23 Helium4 3-dimensional analysis from LET-C
2.800 - 8.000 MeV/n energy range
----------------------------------
HELIUMFLUX24 Helium4 3-dimensional analysis from LET-D
2.800 - 8.000 MeV/n energy range
----------------------------------
----------------------------------
HET event type RATES (for flux calculations) :
----------------------------------
* NOMINAL COINCIDENCE CONDITION status
* exists unless otherwise noted.
* To interpret the LOGIC EQUATIONS (refer to simplistic telescope
* diagrams above) : EXAMPLE: BRIBSP (the BR pre-mnemonic
* indicates to our system a rate bin request and is left here for
* documentation purposes only)
* B1.B2.^SB.^C1.^G1.^A2
* The above LOGIC EQUATION means: a particle entered the
* telescope from the B end, and met the coincidence condition of
* passing through B1, stopping in either B2 or the C432 stack,
* but NOT (= ^ ) tripping the Slant threshold condition SB,
* NOT going into C1, Guard G1, or A2.
*
----------------------------------
HET-I event type rates (for flux calculations) :
----------------------------------
BRIAS A-Stopping High Gain
A1.A2.^C4.^G1.^B2
BRIASZ3 A-Stopping Low Gain Atomic Number
Z >= 3
A1.A2.SA.^C4.^G3.^B2
BRIBSE B-Stopping electron event
B1.B2.C4.^SB.^C1.^G1.^A2
BRIBSP B-Stopping High Gain
B1.B2.SB.^C1.^G1.^A2
BRIBSZ2 B-Stopping Low Gain Atomic Number
Z >= 2
B1.B2.SB.^C1.^G3.^A2
BRIPENH B-Penetrating High Gain
B1.B2.C1
BRIPENL B-Penetrating Low Gain
B1.B2.C1
BRIPGH Guard High Gain
B1.B2.C1.^G1
BRIPGL Guard Low Gain
B1.B2.C1.^G1
BRIBS4E
B1.B2.C4.^C3.^SB.^G1 Stop in C4, did NOT get into C3
BRIBS4P
B1.B2.C4.^C3.SB.^G1 " , High
Gain
BRIBS4
B1.B2.C4.^C3.^SB.^G1 "
BRIBS4Z2
B1.B2.C4.^C3.SB.^G1 " , Low
Gain
BRIBS3E
B1.B2.C4.C3.^C2.^SB.^G1 Stop in C3, did NOT get into C2, High
Gain
BRIBS3P
B1.B2.C4.C3.^C2.SB.^G1 "
BRIBS3
B1.B2.C4.C3.^C2.^SB.^G1 "
BRIBS3Z2
B1.B2.C4.C3.^C2.SB.^G1 " , Low
Gain
BRIBS2E
B1.B2.C4.C3.C2.^C1.^SB.^G1 Stop in C2, did NOT get into C1, High
Gain
BRIBS2P
B1.B2.C4.C3.C2.^C1.SB.^G1 "
BRIBS2
B1.B2.C4.C3.C2.^C1.^SB.^G1 "
BRIBS2Z2
B1.B2.C4.C3.C2.^C1.SB.^G1 " , Low
Gain
----------------------------------
HET-II event type RATES (for flux calculations) :
interpreted analagously to HET-I
----------------------------------
BRIIAS
A1.A2.^C4.^G1.^B2
BRIIASZ3
A1.A2.SA.^C4.^G3.^B2
BRIIBSE
B1.B2.C4.^SB.^C1.^G1.^A2
BRIIBSP
B1.B2.SB.^C1.^G1.^A2
BRIIBSZ2
B1.B2.SB.^C1.^G3.^A2
BRIIPENH
B1.B2.C1
BRIIPENL
B1.B2.C1
BRIIPGH
B1.B2.C1.^G1
BRIIPGL
B1.B2.C1.^G1
BRIIBS4E
B1.B2.C4.^C3.^SB.^G1
BRIIBS4P
B1.B2.C4.^C3.SB.^G1
BRIIBS4
B1.B2.C4.^C3.^SB.^G1
BRIIBS4Z2
B1.B2.C4.^C3.SB.^G1
BRIIBS3E
B1.B2.C4.C3.^C2.^SB.^G1
BRIIBS3P
B1.B2.C4.C3.^C2.SB.^G1
BRIIBS3
B1.B2.C4.C3.^C2.^SB.^G1
BRIIBS3Z2
B1.B2.C4.C3.^C2.SB.^G1
BRIIBS2E
B1.B2.C4.C3.C2.^C1.^SB.^G1
BRIIBS2P
B1.B2.C4.C3.C2.^C1.SB.^G1
BRIIBS2
B1.B2.C4.C3.C2.^C1.^SB.^G1
BRIIBS2Z2
B1.B2.C4.C3.C2.^C1.SB.^G1
----------------------------------
HET-I singles rates
----------------------------------
BRIA1H Singles rate, high gain, for the A1
A1 element
below are all high gain until noted
BRIA2H
A2
BRIC1H
C1
BRIC2H
C2
BRIB1H
B1
BRISBH
SB
BRIC3H
C3
BRIC4H
C4
BRIB2H
B2
BRIG1
G1
BRIA1L begin low gain singles here
A1
BRIA2L
A2
BRIC1L
C1
BRIC2L
C2
BRIB1L
B1
BRISA1
SA
BRISA2
SA
BRISBL
SB
BRIC3L
C3
BRIC4L
C4
BRIB2L
B2
----------------------------------
HET-II singles rates
Interpreted the same as HET-I singles rates
----------------------------------
BRIIA1H
A1
BRIIA2H
A2
BRIIC1H
C1
BRIIC2H
C2
BRIIB1H
B1
BRIISBH
SB
BRIIC3H
C3
BRIIC4H
C4
BRIIB2H
B2
BRIIG1
G1
BRIIA1L begin low gain singles here
A1
BRIIA2L
A2
BRIIC1L
C1
BRIIC2L
C2
BRIIB1L
B1
BRIISA1
SA
BRIISA2
SA
BRIISBL
SB
BRIIC3L
C3
BRIIC4L
C4
BRIIB2L
B2
----------------------------------
LET singles rates in high gain
----------------------------------
BRLA1
L1
BRLA2
L2
BRLA3
L3
BRLA4
L4
BRSLA
SL
BRSLB
SL
BRLB1
L1
BRLB2
L2
BRLB3
L3
BRLB4
L4
BRLC1
L1
BRLC2
L2
BRLC3
L3
BRLC4
L4
BRSLD
SL
BRLD1
L1
BRLD2
L2
BRLD3
L3
BRLD4
L4
----------------------------------
TET singles rates H or L at end of rate indicates High or Low Gain
----------------------------------
BRD6L
D6
BRGA+GB
GA.GB
BRD5H
D5
BRD7L
D7
BRD6H
D6
BRD7H
D7
BRD5L
D5
BRD8L
D8
BRD1H
D1
BRD4H
D4
BRD2L
D2
BRD3L
D3
BRD1L
D1
BRD3H
D3
BRD2H
D2
BRD4L
D4
* MAJOR STATUS CHANGE CONFIGURATIONS IN CRUISE AFFECT THESE
----------------------------------
LET event type rates (for flux calculations) :
----------------------------------
BRLATRP
L1.L2.^L4
BRLBTRP
L1.L2.^L4
BRLCTRP
L1.L2.L3.^L4
BRLCTRP
L1.L2.^L4
BRLDTRP
L1.L2.^L4
BRLC High Gain (typical mnemonic)
L1.L2.L3.^SL.^L4
BRLC
L1.L2.^SL.^L4
BRLCZ3 Low Gain Atomic Number Z >= 3
L1.L2.L3.SL.^L4 (typical mnemonic)
BRLCZ3
L1.L2.SL.^L4
BRLD
L1.L2.L3.^SL.^L4
BRLD
L1.L2.^SL.^L4
BRLDZ3
L1.L2.L3.SL.^L4
BRLDZ3
L1.L2.SL.^L4
BRLA
L1.L2.^SL.^L4
BRLAZ3
L1.L2.SL.^L4
BRLB
L1.L2.^SL.^L4
BRLBZ3
L1.L2.SL.^L4
----------------------------------
TET event type rates (for flux calculations) :
----------------------------------
BRTAN
W1.W2.D3.^D8.^GA.^GB
BRTAN
W1.W2.^D8.^GA.^GB
BRTLO
W1.W2.D3.D5.^D6.^GA.^GB.^UT
BRTLO
W1.W2.D5.^D6.^GA.^GB.^UT
BRTHI
W1.W2.D3.D7.^D8.^GA.^GB.^UT
BRTHI
W1.W2.D7.^D8.^GA.^GB.^UT
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The following is a list of the exact data quantities we have included in the NSSDC COHO database for the time period: Launch - 06/29/79. See above for the basic description of these quantities.
* - SET 1 WILL BE AUTOGAIN MODE, VERY SIMILAR TO V1FBINS
* LAUNCH - JUPITER USE ~6/29/79
TIME,
HELIUMFLUX1,
HELIUMFLUX2,
HELIUMFLUX3,
HELIUMFLUX4,
HELIUMFLUX5,
HELIUMFLUX6,
HELIUMFLUX7,
HELIUMFLUX8,
PROTONFLUX1,
PROTONFLUX2,
PROTONFLUX3,
PROTONFLUX4,
PROTONFLUX5,
HELIUMFLUX9,
HELIUMFLUX10,
HELIUMFLUX11,
HELIUMFLUX12,
HELIUMFLUX13,
HELIUMFLUX14,
HELIUMFLUX15,
HELIUMFLUX16,
PROTONFLUX6,
PROTONFLUX7,
PROTONFLUX8,
PROTONFLUX9,
PROTONFLUX10,
PROTONFLUX11,
PROTONFLUX12,
PROTONFLUX13,
PROTONFLUX14,
PROTONFLUX15,
PROTONFLUX16,
PROTONFLUX17,
PROTONFLUX18,
HELIUMFLUX17,
HELIUMFLUX18,
HELIUMFLUX19,
HELIUMFLUX20,
HELIUMFLUX21,
HELIUMFLUX22,
HELIUMFLUX23,
HELIUMFLUX24,
BRIAS .
BRIASZ3 .
BRIBSE .
BRIBSP .
BRIBSZ2 .
BRIPENL .
BRIPENH .
BRIPGL .
BRIPGH .
BRIBS4E .
BRIBS4P .
BRIBS4 .
BRIBS4Z2 .
BRIBS2E .
BRIBS2P .
BRIBS2 .
BRIBS2Z2 .
BRIBS3E .
BRIBS3P .
BRIBS3 .
BRIBS3Z2 .
BRISA1 .
BRISA2 .
BRIG1 .
BRIISA1 .
BRIISA2 .
BRIIG1 .
BRIIAS .
BRIIASZ3 .
BRIIBSE .
BRIIBSP .
BRIIBSZ2 .
BRIIPENL .
BRIIPENH .
BRIIPGL .
BRIIPGH .
BRIIBS4E .
BRIIBS4P .
BRIIBS4 .
BRIIBS4Z2 .
BRIIBS2E .
BRIIBS2P .
BRIIBS2 .
BRIIBS2Z2 .
BRIIBS3E .
BRIIBS3P .
BRIIBS3 .
BRIIBS3Z2 .
BRIA1H .
BRIA2H .
BRIB1H .
BRIB2H .
BRIC1H .
BRIC2H .
BRIC3H .
BRIC4H .
BRISBH .
BRIA1L .
BRIA2L .
BRIB1L .
BRIB2L .
BRIC1L .
BRIC2L .
BRIC3L .
BRIC4L .
BRISBL .
BRIIA1H .
BRIIA2H .
BRIIB1H .
BRIIB2H .
BRIIC1H .
BRIIC2H .
BRIIC3H .
BRIIC4H .
BRIISBH .
BRIIA1L .
BRIIA2L .
BRIIB1L .
BRIIB2L .
BRIIC1L .
BRIIC2L .
BRIIC3L .
BRIIC4L .
BRIISBL .
BRLA1 .
BRLB1 .
BRLC1 .
BRLD1 .
BRLA2 .
BRLB2 .
BRLC2 .
BRLD2 .
BRLA3 .
BRLB3 .
BRLC3 .
BRLD3 .
BRLA4 .
BRLB4 .
BRLC4 .
BRLD4 .
BRSLA .
BRSLB .
BRSLC .
BRSLD .
BRLATRP .
BRLBTRP .
BRLCTRP .
BRLDTRP .
BRD1L .
BRD2L .
BRD3L .
BRD4L .
BRD5L .
BRD6L .
BRD7L .
BRD8L .
BRGA+GB .
BRD1H .
BRD2H .
BRD3H .
BRD4H .
BRD5H .
BRD6H .
BRD7H .
* MAJOR STATUS CHANGE CONFIGURATIONS IN CRUISE AFFECT THESE
BRLC . X
X
L1.L2.L3.^SL.^L4
BRLC . X
X
L1.L2.^SL.^L4
BRLCZ3 . X
X
L1.L2.L3.SL.^L4
BRLCZ3 . X
X
L1.L2.SL.^L4
BRLD . X
X
L1.L2.L3.^SL.^L4
BRLD . X
X
L1.L2.^SL.^L4
BRLDZ3 . X
X
L1.L2.L3.SL.^L4
BRLDZ3 . X
X
L1.L2.SL.^L4
BRLA . X
X
L1.L2.L3.^SL.^L4
BRLA . X
X
L1.L2.^SL.^L4
BRLAZ3 . X
X
L1.L2.L3.SL.^L4
BRLAZ3 . X
X
L1.L2.SL.^L4
BRLB . X
X
L1.L2.L3.^SL.^L4
BRLB . X
X
L1.L2.^SL.^L4
BRLBZ3 . X
X
L1.L2.L3.SL.^L4
BRLBZ3 . X
X
L1.L2.SL.^L4
BRTAN . X
X
W1.W2.D3.^D8.^GA.^GB
BRTAN . X
X
W1.W2.^D8.^GA.^GB
BRTLO .
BRTLO . X
X
W1.W2.D5.^D6.^GA.^GB.^UT
BRTHI .
BRTHI . X
X
W1.W2.D7.^D8.^GA.^GB.^UT
Return to the top of this page.
Return to the Voyager Cosmic Ray Subsytem page.
The following is a list of the exact data quantities we have included in the NSSDC COHO database for the time period: 08/22/79 - 04/22/82. See above for the basic description of these quantities.
* - SET 2 HAS HET I GAIN SET HIGH WITH CYCLING OF THAT AND OTHER
* 8/22/79 19:30 - 10/24/97 CYCLING OF SOME WORDS
* 10/24/79 17:30 - 10/20/81 22:45 STABLE
* 10/20/81 22:45 - 4/21/82 17:30 CYCLINGS VARIOUS
TIME,
HELIUMFLUX1,
HELIUMFLUX2,
HELIUMFLUX5,
HELIUMFLUX6,
HELIUMFLUX8,
PROTONFLUX1,
PROTONFLUX2,
PROTONFLUX3,
PROTONFLUX4,
PROTONFLUX5,
HELIUMFLUX11,
HELIUMFLUX12,
HELIUMFLUX15,
PROTONFLUX11,
PROTONFLUX13,
PROTONFLUX14,
PROTONFLUX15,
PROTONFLUX17,
PROTONFLUX18,
HELIUMFLUX17,
HELIUMFLUX19,
HELIUMFLUX20,
HELIUMFLUX21,
HELIUMFLUX23,
HELIUMFLUX24,
* LOW GAIN OUT *R in colums 1,2 indicates not present
BRIAS .
*RIASZ3 .
BRIBSE .
BRIBSP .
*RIBSZ2 .
*RIPENL .
BRIPENH .
*RIPGL .
BRIPGH .
BRIBS4E .
BRIBS4P .
*RIBS4 .
*RIBS4Z2 .
BRIBS2E .
BRIBS2P .
*RIBS2 .
*RIBS2Z2 .
BRIBS3E .
BRIBS3P .
*RIBS3 .
*RIBS3Z2 .
BRISA1 .
BRISA2 .
BRIG1 .
* II LOW GAIN ONLY
BRIISA1 .
BRIISA2 .
BRIIG1 .
*RIIAS .
BRIIASZ3 .
*RIIBSE .
*RIIBSP .
BRIIBSZ2 .
BRIIPENL .
*RIIPENH .
BRIIPGL .
*RIIPGH .
*RIIBS4E .
*RIIBS4P .
BRIIBS4 .
BRIIBS4Z2 .
*RIIBS2E .
*RIIBS2P .
BRIIBS2 .
BRIIBS2Z2 .
*RIIBS3E .
*RIIBS3P .
BRIIBS3 .
BRIIBS3Z2 .
* I HIGH GAIN ONLY II LOW GAIN ONLY
BRIA1H .
BRIA2H .
BRIB1H .
BRIB2H .
BRIC1H .
BRIC2H .
BRIC3H .
BRIC4H .
BRISBH .
*RIA1L .
*RIA2L .
*RIB1L .
*RIB2L .
*RIC1L .
*RIC2L .
*RIC3L .
*RIC4L .
*RISBL .
*RIIA1H .
*RIIA2H .
*RIIB1H .
*RIIB2H .
*RIIC1H .
*RIIC2H .
*RIIC3H .
*RIIC4H .
*RIISBH .
BRIIA1L .
BRIIA2L .
BRIIB1L .
BRIIB2L .
BRIIC1L .
BRIIC2L .
BRIIC3L .
BRIIC4L .
BRIISBL .
BRLA1 .
*RLB1 .
BRLC1 .
BRLD1 .
BRLA2 .
BRLB2 .
BRLC2 .
BRLD2 .
BRLA3 .
BRLB3 .
BRLC3 .
BRLD3 .
BRLA4 .
BRLB4 .
BRLC4 .
BRLD4 .
BRSLA .
BRSLB .
BRSLC .
BRSLD .
BRLATRP .
BRLBTRP .
BRLCTRP .
BRLDTRP .
BRD1L .
BRD2L .
BRD3L .
BRD4L .
BRD5L .
BRD6L .
BRD7L .
BRD8L .
BRGA+GB .
BRD1H .
BRD2H .
BRD3H .
BRD4H .
BRD5H .
BRD6H .
BRD7H .
* MAJOR STATUS CHANGE CONFIGURATIONS IN CRUISE AFFECT THESE
BRLC . X
X
L1.L2.L3.^SL.^L4
BRLC . X
X
L1.L2.^SL.^L4
BRLCZ3 . X
X
L1.L2.L3.SL.^L4
BRLCZ3 . X
X
L1.L2.SL.^L4
BRLD . X
X
L1.L2.L3.^SL.^L4
BRLD . X
X
L1.L2.^SL.^L4
BRLDZ3 . X
X
L1.L2.L3.SL.^L4
BRLDZ3 . X
X
L1.L2.SL.^L4
BRLA . X
X
L1.L2.L3.^SL.^L4
BRLA . X
X
L1.L2.^SL.^L4
BRLAZ3 . X
X
L1.L2.L3.SL.^L4
BRLAZ3 . X
X
L1.L2.SL.^L4
BRLB . X
X
L1.L2.L3.^SL.^L4
BRLB . X
X
L1.L2.^SL.^L4
BRLBZ3 . X
X
L1.L2.L3.SL.^L4
BRLBZ3 . X
X
L1.L2.SL.^L4
BRTAN . X
X
W1.W2.D3.^D8.^GA.^GB
BRTAN . X
X
W1.W2.^D8.^GA.^GB
BRTLO .
BRTLO . X
X
W1.W2.D5.^D6.^GA.^GB.^UT
BRTHI .
BRTHI . X
X
W1.W2.D7.^D8.^GA.^GB.^UT
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The following is a list of the exact data quantities we have included in the NSSDC COHO database for the time period: 04/22/82 - 12/31/92. See above for the basic description of these quantities.
* - SET 3 HAS HET I GAIN SET HIGH AND OTHER STABLE
* 4/21/82 17:30 - EOD EXCEPT FOR TAN TO NOMINAL AT 3/12/85
TIME,
HELIUMFLUX1,
HELIUMFLUX2,
HELIUMFLUX5,
HELIUMFLUX6,
HELIUMFLUX8,
PROTONFLUX1,
PROTONFLUX2,
PROTONFLUX3,
PROTONFLUX4,
PROTONFLUX5,
HELIUMFLUX11,
HELIUMFLUX12,
HELIUMFLUX15,
PROTONFLUX11,
PROTONFLUX13,
PROTONFLUX14,
PROTONFLUX15,
PROTONFLUX17,
PROTONFLUX18,
HELIUMFLUX17,
HELIUMFLUX19,
HELIUMFLUX20,
HELIUMFLUX21,
HELIUMFLUX23,
HELIUMFLUX24,
* LOW GAIN OUT *R in cols 1,2 indicates not present
BRIAS .
*RIASZ3 .
BRIBSE .
BRIBSP .
*RIBSZ2 .
*RIPENL .
BRIPENH .
*RIPGL .
BRIPGH .
BRIBS4E .
BRIBS4P .
*RIBS4 .
*RIBS4Z2 .
BRIBS2E .
BRIBS2P .
*RIBS2 .
*RIBS2Z2 .
BRIBS3E .
BRIBS3P .
*RIBS3 .
*RIBS3Z2 .
* THESE 3 OUT BECAUSE OF G1 BIT STUCK PROBLEM AND THEY ARE LOW GAIN
*RISA1 .
*RISA2 .
*RIG1 .
* II LOW GAIN ONLY
BRIISA1 .
BRIISA2 .
BRIIG1 .
*RIIAS .
BRIIASZ3 .
*RIIBSE .
*RIIBSP .
BRIIBSZ2 .
BRIIPENL .
*RIIPENH .
BRIIPGL .
*RIIPGH .
*RIIBS4E .
*RIIBS4P .
BRIIBS4 .
BRIIBS4Z2 .
*RIIBS2E .
*RIIBS2P .
BRIIBS2 .
BRIIBS2Z2 .
*RIIBS3E .
*RIIBS3P .
BRIIBS3 .
BRIIBS3Z2 .
* I HIGH GAIN ONLY II LOW GAIN ONLY
BRIA1H .
BRIA2H .
BRIB1H .
BRIB2H .
BRIC1H .
BRIC2H .
BRIC3H .
BRIC4H .
BRISBH .
*RIA1L .
*RIA2L .
*RIB1L .
*RIB2L .
*RIC1L .
*RIC2L .
*RIC3L .
*RIC4L .
*RISBL .
*RIIA1H .
*RIIA2H .
*RIIB1H .
*RIIB2H .
*RIIC1H .
*RIIC2H .
*RIIC3H .
*RIIC4H .
*RIISBH .
BRIIA1L .
BRIIA2L .
BRIIB1L .
BRIIB2L .
BRIIC1L .
BRIIC2L .
BRIIC3L .
BRIIC4L .
BRIISBL .
BRLA1 .
*RLB1 .
BRLC1 .
BRLD1 .
BRLA2 .
BRLB2 .
BRLC2 .
BRLD2 .
BRLA3 .
BRLB3 .
BRLC3 .
BRLD3 .
BRLA4 .
BRLB4 .
BRLC4 .
BRLD4 .
BRSLA .
BRSLB .
BRSLC .
BRSLD .
BRLATRP .
*RLBTRP .
BRLCTRP .
BRLDTRP .
BRD1L .
BRD2L .
BRD3L .
BRD4L .
BRD5L .
BRD6L .
BRD7L .
BRD8L .
BRGA+GB .
BRD1H .
BRD2H .
BRD3H .
BRD4H .
BRD5H .
BRD6H .
BRD7H .
* MAJOR STATUS CHANGE CONFIGURATIONS IN CRUISE AFFECT THESE
BRLC . X
X
L1.L2.L3.^SL.^L4
BRLC . X
X
L1.L2.^SL.^L4
BRLCZ3 . X
X
L1.L2.L3.SL.^L4
BRLCZ3 . X
X
L1.L2.SL.^L4
BRLD . X
X
L1.L2.L3.^SL.^L4
BRLD . X
X
L1.L2.^SL.^L4
BRLDZ3 . X
X
L1.L2.L3.SL.^L4
BRLDZ3 . X
X
L1.L2.SL.^L4
BRLA . X
X
L1.L2.L3.^SL.^L4
BRLA . X
X
L1.L2.^SL.^L4
BRLAZ3 . X
X
L1.L2.L3.SL.^L4
BRLAZ3 . X
X
L1.L2.SL.^L4
*RLB . X
* X
* L1.L2.L3.^SL.^L4
*RLB . X
* X
* L1.L2.^SL.^L4
*RLBZ3 . X
* X
* L1.L2.L3.SL.^L4
*RLBZ3 . X
* X
* L1.L2.SL.^L4
BRTAN . X
X
W1.W2.D3.^D8.^GA.^GB
BRTAN . X
X
W1.W2.^D8.^GA.^GB
BRTLO .
BRTLO . X
X
W1.W2.D5.^D6.^GA.^GB.^UT
BRTHI .
BRTHI . X
X
W1.W2.D7.^D8.^GA.^GB.^UT
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