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Fundamental TechnologiesVoyager LECP Pages |
STEP and STEPF Files
Definitions and Naming Convention
The files are prepared from the FAT (STEP) and filtered FAT (STEPF) binary files. The FAT files are step-synchronous averages of the LECP data. All data samples that occur within a specific motor position are averaged. If no data are read out in a given motor position, the datum will be absent. This file has one record for each motor position. If the LECP instrument is parked, then records are generated every 24 seconds with the motor position unchanging. Filtered FAT files are generated by comparing the rates derived from the MRT files with a “reasonable” maximum rate. Data that exceed the expected maximum are omitted from the averages.
First Line Sample: VOYAGER1,PRINTED,10-AUG-01,15:18:12,V177250A76.lst
(START)YYYY DD HH MM SEC (STOP) YYY DD HH MM SEC SECTOR N*(Item, Unc.)
where N* repeats the item and its uncertainty. The files are created in two systems of units, rates
and fluxes. The naming conventions for these files are:
SSYYDDD(G,F)SGG.LST or SSYYDDDSGG.CSV where:
SS = V1 or V2
YY = two digit year number (77 through Present)
DDD = three digit day of year (for file start time)
(G,F) is an
optional character which is present in the STEPF files to indicate that
filtering has been applied
“S” = Stands for ASCII Listing of “Step” Files
GG = Group number from table below.
|
Grp. # |
Col. 1 |
Col.2 |
Col. 3 |
Col.3 |
Col. 5 |
Col. 6 |
Descriptions |
|
1 |
18 |
19 |
20 |
21 |
22 |
PL01,2,3,4,5 Rates |
|
|
2 |
23 |
24 |
25 |
44 |
45 |
PL06,7,8,AL01,2 Rates |
|
|
3 |
1 |
3 |
5 |
7 |
9 |
EB01,2,3,4,5 Rates |
|
|
4 |
2 |
4 |
6 |
8 |
10 |
EB'01,2,3,4,5 Rates |
|
|
5 |
11 |
12 |
13 |
14 |
EG06,7,8,9 Rates |
||
|
6 |
34 |
50 |
36 |
52 |
E0 (E1) , D1F1, D1F2 Rates |
||
|
7 |
26 |
35 |
46 |
51 |
60 |
E0 E2 (E3) Rates |
|
|
8 |
27 |
28 |
29 |
53 |
54 |
Protons, Mediums Rates |
|
|
9 |
37 |
38 |
47 |
61 |
62 |
Alphas, L Nuclei, H Nuclei Rates |
|
|
10 |
39 |
40 |
48 |
55 |
63 |
Alphas, L Nuclei, H Nuclei Rates |
|
|
11 |
15 |
16 |
17 |
33 |
E44, E45, E37, P31 Rates |
||
|
12 |
30 |
31 |
42 |
58 |
66 |
E5 E4 (E3) Rates |
|
|
13 |
32 |
43 |
59 |
67 |
E5 E4 E3 E2 Rates |
||
|
14 |
41 |
49 |
56 |
57 |
64 |
65 |
E5 E4 (E3) Rates |
|
15 |
68 |
75 |
76 |
74 |
73 |
Singles Rates |
|
|
16 |
69 |
70 |
71 |
72 |
Singles Rates |
||
|
17 |
83 |
84 |
85 |
97 |
98 |
99 |
P d09,10,11, A d03,04,Z d01 Rates |
|
18 |
80 |
81 |
82 |
94 |
95 |
96 |
P d’09,10,11, A d’03,04,Z d’01 Rates |
|
19 |
77 |
88 |
89 |
90 |
ESA0, PSA1, PSA2, PSA3 Rates |
||
|
20 |
78 |
91 |
92 |
93 |
ESB0, PSB1, PSB2, PSB3 Rates |
||
|
21 |
79 |
86 |
87 |
AB10, AB12, AB13 Rates |
|||
|
22 |
18 |
19 |
20 |
21 |
22 |
PL01,2,3,4,5 Fluxes |
|
|
23 |
23 |
24 |
25 |
44 |
45 |
PL06,7,8,AL01,2 Fluxes |
|
|
24 |
1 |
3 |
5 |
7 |
9 |
EB01,2,3,4,5 Fluxes |
|
|
25 |
2 |
4 |
6 |
8 |
10 |
EB'01,2,3,4,5 Fluxes |
|
|
26 |
11 |
12 |
13 |
14 |
EG06,7,8,9 Fluxes |
||
|
27 |
34 |
50 |
36 |
52 |
E0 (E1) , D1F1, D1F2 Fluxes |
||
|
28 |
26 |
35 |
46 |
51 |
60 |
E0 E2 (E3) Fluxes |
|
|
29 |
27 |
28 |
29 |
53 |
54 |
Protons, Mediums Fluxes |
|
|
30 |
37 |
38 |
47 |
61 |
62 |
Alphas, L Nuclei, H Nuclei Fluxes |
|
|
31 |
39 |
40 |
48 |
55 |
63 |
Alphas, L Nuclei, H Nuclei Fluxes |
|
|
32 |
15 |
16 |
17 |
33 |
E44, E45, E37, P31 Fluxes |
||
|
33 |
30 |
31 |
42 |
58 |
66 |
E5 E4 (E3) Fluxes |
|
|
34 |
32 |
43 |
59 |
67 |
E5 E4 E3 E2 Fluxes |
||
|
35 |
41 |
49 |
56 |
57 |
64 |
65 |
E5 E4 (E3) Fluxes |
|
36 |
83 |
84 |
85 |
97 |
98 |
99 |
P d09,10,11, A d03,04,Z d01 Fluxes |
|
37 |
80 |
81 |
82 |
94 |
95 |
96 |
P d’09,10,11, A d’03,04,Z d’01 Fluxes |
|
38 |
77 |
88 |
89 |
90 |
ESA0, PSA1, PSA2, PSA3 Fluxes |
||
|
39 |
78 |
91 |
92 |
93 |
ESB0, PSB1, PSB2, PSB3 Fluxes |
||
|
40 |
79 |
86 |
87 |
AB10, AB12, AB13 Fluxes |
Passbands and Geometrical Factors for
Voyager 1 LECP Far Encounter and Cruise Channels
Passbands and Geometrical Factors for
Voyager 2 LECP Far Encounter and Cruise Channels
|
INDEX |
FAT # |
NAME |
LOW |
HIGH |
MEAN |
G.F. (cm2sr) |
|
1 |
1. |
EB01 |
0.015 |
0.0370 |
0.020 |
0.006 |
|
2 |
2. |
EBD1 |
0.015 |
0.5000 |
0.020 |
0.00012 |
|
3 |
3. |
EB02 |
0.037 |
0.0610 |
0.045 |
0.006 |
|
4 |
4. |
EBD2 |
0.037 |
0.5000 |
0.045 |
0.00012 |
|
5 |
5. |
EB03 |
0.070 |
0.112 |
0.090 |
0.006 |
|
6 |
6. |
EBD3 |
0.070 |
0.5000 |
0.090 |
0.00012 |
|
7 |
7. |
EB04 |
0.130 |
0.1830 |
0.120 |
0.006 |
|
8 |
8. |
EBD4 |
0.130 |
0.5000 |
0.120 |
0.00012 |
|
9 |
9. |
EB05 |
0.200 |
0.5000 |
0.200 |
0.006 |
|
10 |
10. |
EBD5 |
0.200 |
0.5000 |
0.200 |
0.00012 |
|
11 |
11. |
EG06 |
0.252 |
2.0000 |
0.250 |
0.00200 |
|
12 |
12. |
EG07 |
0.480 |
2.0000 |
0.500 |
0.00200 |
|
13 |
13. |
EG08 |
0.853 |
2.0000 |
0.900 |
0.00200 |
|
14 |
14. |
EG09 |
2.100 |
5.0000 |
2.000 |
0.00200 |
|
15 |
|
|
|
|
|
|
|
16 |
|
|
|
|
|
|
|
17 |
|
|
|
|
|
|
|
18 |
18. |
PL01 |
0.030 |
0.0530 |
0.025 |
0.04020 |
|
19 |
19. |
PL02 |
0.053 |
0.0850 |
0.050 |
0.04020 |
|
20 |
20. |
PL03 |
0.085 |
0.1390 |
0.100 |
0.04020 |
|
21 |
21. |
PL04 |
0.139 |
0.2000 |
0.150 |
0.04020 |
|
22 |
22. |
PL05 |
0.2000 |
0.5500 |
0.2500 |
0.04020 |
|
23 |
23. |
PL06 |
0.5400 |
1.0500 |
0.6 |
0.04020 |
|
24 |
24. |
PL07 |
1.0500 |
2.0300 |
1.0000 |
0.04020 |
|
25 |
25. |
PL08 |
2.0300 |
4.0100 |
2.5000 |
0.04020 |
|
26 |
44. |
AL01 |
0.9800 |
1.7700 |
1.0000 |
0.04020 |
|
27 |
45. |
AL02 |
1.7700 |
4.2200 |
2.5000 |
0.04020 |
|
28 |
77. |
ESA0 |
2.5000 |
99.999 |
2.5000 |
0.49350 |
|
29 |
78. |
ESB0 |
8.5000 |
99.999 |
8.5000 |
0.94620 |
|
30 |
79. |
AB10 |
8.5000 |
99.999 |
8.5000 |
0.05040 |
|
31 |
80. |
DP09 |
0.2850 |
5.0200 |
0.2500 |
0.00084 |
|
32 |
81. |
DP10 |
0.4800 |
2.5800 |
0.6 |
0.00084 |
|
33 |
82. |
DP11 |
0.7250 |
1.6400 |
1.0000 |
0.00084 |
|
34 |
83. |
PD09 |
0.2850 |
5.2500 |
0.2500 |
0.00260 |
|
35 |
84. |
PD10 |
0.4800 |
2.7200 |
0.6 |
0.00260 |
|
36 |
85. |
PD11 |
0.7250 |
1.5800 |
1.0000 |
0.00260 |
|
37 |
86. |
AB12 |
54.000 |
87.300 |
50.000 |
0.05040 |
|
38 |
87. |
AB13 |
87.300 |
152.00 |
100.00 |
0.05040 |
|
39 |
88. |
PSA1 |
15.800 |
158.00 |
15.000 |
0.49350 |
|
40 |
89. |
PSA2 |
15.800 |
49.000 |
25.000 |
0.49350 |
|
41 |
90. |
PSA3 |
16.300 |
26.200 |
25.000 |
0.49350 |
|
42 |