# { # "OriginFile": { "DESCRIPTION": "ViRBO origin file for Qin-Denton data", # "NAME": "OriginFile", # "VALUES": [""]}, # # "DateTime": { "DESCRIPTION": "The date and time in ISO 8601 compliant format.", # "NAME": "IsoDateTime", # "TITLE": "ISO DateTime", # "LABEL": "Time", # "UNITS": "UTC", # "START_COLUMN": 0 }, # # "Year": { "DESCRIPTION": "Year.", # "NAME": "Year", # "TITLE": "Year", # "LABEL": "Year", # "START_COLUMN": 1, # "UNITS": "Years" }, # # "Month": { "DESCRIPTION": "Month", # "NAME": "Month", # "TITLE": "Month", # "LABEL": "Month", # "START_COLUMN": 2, # "UNITS": "Months"}, # # "Day": { "DESCRIPTION": "Day of month.", # "NAME": "Day", # "TITLE": "Day", # "LABEL": "Day", # "START_COLUMN": 3, # "UNITS": "Days" }, # # "Hour": { "DESCRIPTION": "Hour of current day.", # "NAME": "Hours", # "TITLE": "Hours", # "LABEL": "Hours", # "START_COLUMN": 4, # "UNITS": "Hours" }, # # "Minute": { "DESCRIPTION": "Minute of the current hour.", # "NAME": "Minutes", # "TITLE": "Minutes", # "LABEL": "Minutes", # "START_COLUMN": 5, # "UNITS": "Minutes" }, # # "Second": { "DESCRIPTION": "Second of the current minute.", # "NAME": "Seconds", # "TITLE": "Seconds", # "LABEL": "Seconds", # "START_COLUMN": 6, # "UNITS": "Seconds" }, # # "ByIMF": { "DESCRIPTION": "Y-component of the interplanetary magnetic field.", # "NAME": "ByIMF", # "TITLE": "IMF By", # "LABEL": "IMF B!By!N, nT", # "START_COLUMN": 7, # "UNITS": "nT" }, # # "BzIMF": { "DESCRIPTION": "Z-component of the interplanetary magnetic field.", # "NAME": "BzIMF", # "TITLE": "IMF Bz", # "LABEL": "IMF B!Bz!N, nT", # "START_COLUMN": 8, # "UNITS": "nT" }, # # "Vsw": { "DESCRIPTION": "Solar wind speed.", # "NAME": "Vsw", # "TITLE": "Solar Wind Speed", # "LABEL": "V!BSW!N, km/s", # "START_COLUMN": 9, # "UNITS": "km/s" }, # # "Den_P": { "DESCRIPTION": "Solar wind proton density.", # "NAME": "Den_P", # "TITLE": "Solar Wind Proton Density", # "LABEL": "N!Bp!N, cm!E-3!N", # "START_COLUMN": 10, # "UNITS": "cm^-3" }, # # "Pdyn": { "DESCRIPTION": "Solar wind dynamic pressure.", # "NAME": "Pdyn", # "TITLE": "Solar Wind Dynamic Pressure", # "LABEL": "P!Bdyn!N, nPa", # "START_COLUMN": 11, # "UNITS": "nPa" }, # # "G": { "DESCRIPTION": "Tsyganenko G parameters.", # "NAME": "G", # "TITLE": "Tsyganenko G parameters", # "LABEL": "Tsyganenko G!Bi!N", # "DIMENSION": [ 3 ], # "START_COLUMN": 12, # "ELEMENT_NAMES": [ "G1", "G2", "G3" ], # "ELEMENT_LABELS": [ "G1", "G2", "G3" ] }, # # "ByIMF_status": { "DESCRIPTION": "Quality flag for ByIMF value.", # "NAME": "ByIMF_status", # "TITLE": "ByIMF_status", # "LABEL": "ByIMF_status", # "START_COLUMN": 15, # "UNITS": "dimless" }, # # "BzIMF_status": { "DESCRIPTION": "Quality flag for BzIMF value.", # "NAME": "BzIMF_status", # "TITLE": "BzIMF_status", # "LABEL": "BzIMF_status", # "START_COLUMN": 16, # "UNITS": "dimless" }, # # "Vsw_status": { "DESCRIPTION": "Quality flag for Vsw value.", # "NAME": "Vsw_status", # "TITLE": "Vsw_status", # "LABEL": "Vsw_status", # "START_COLUMN": 17, # "UNITS": "dimless" }, # # "Den_P_status": { "DESCRIPTION": "Quality flag for Den_P value.", # "NAME": "Den_P_status", # "TITLE": "Den_P_status", # "LABEL": "Den_P_status", # "START_COLUMN": 18, # "UNITS": "dimless" }, # # "Pdyn_status": { "DESCRIPTION": "Quality flag for Pdyn value.", # "NAME": "Pdyn_status", # "TITLE": "Pdyn_status", # "LABEL": "Pdyn_status", # "START_COLUMN": 19, # "UNITS": "dimless" }, # # "G_status": { "DESCRIPTION": "Quality flag for G values.", # "NAME": "G_status", # "TITLE": "G_status", # "LABEL": "G_status", # "DIMENSION": [ 3 ], # "START_COLUMN": 20, # "ELEMENT_NAMES": [ "G1_status", "G2_status", "G3_status" ], # "ELEMENT_LABELS": [ "dimless", "dimless", "dimless" ] }, # # # "Kp": { "DESCRIPTION": "Kp index.", # "NAME": "Kp", # "TITLE": "Kp Index", # "LABEL": "Kp", # "START_COLUMN": 23, # "UNITS": "dimless" }, # # "akp3": { "DESCRIPTION": "akp3 index.", # "NAME": "akp3", # "TITLE": "akp3 Index", # "LABEL": "akp3", # "START_COLUMN": 24, # "UNITS": "dimless" }, # # "Dst": { "DESCRIPTION": "Dst index.", # "NAME": "Dst", # "TITLE": "Dst Index", # "LABEL": "Dst, nT", # "START_COLUMN": 25, # "UNITS": "nT" }, # # "Bz": { "DESCRIPTION": "Tsyganenko Bz parameters.", # "NAME": "Bz", # "TITLE": "Tsyganenko Bz parameters", # "LABEL": "Bz!Bi!N, nT", # "DIMENSION": [ 6 ], # "START_COLUMN": 26, # "ELEMENT_NAMES": [ "Bz1", "Bz2", "Bz3", "Bz4", "Bz5", "Bz6" ], # "ELEMENT_LABELS": [ "Bz1", "Bz2", "Bz3", "Bz4", "Bz5", "Bz6" ] }, # # "W": { "DESCRIPTION": "Tsyganenko W parameters.", # "NAME": "W", # "TITLE": "Tsyganenko W parameters", # "LABEL": "Tsyganenko W!Bi!N", # "DIMENSION": [ 6 ], # "START_COLUMN": 32, # "ELEMENT_NAMES": [ "W1", "W2", "W3", "W4", "W5", "W6" ], # "ELEMENT_LABELS": [ "W1", "W2", "W3", "W4", "W5", "W6" ] }, # # "W_status": { "DESCRIPTION": "Quality flags for Tsyganeko W parameters.", # "NAME": "W_status", # "TITLE": "Tsyganenko W_status parameters", # "LABEL": "Tsyganenko W!Bi!N_status", # "DIMENSION": [ 6 ], # "START_COLUMN": 38, # "ELEMENT_NAMES": [ "W1_status", "W2_status", "W3_status", "W4_status", "W5_status", "W6_status" ], # "ELEMENT_LABELS": [ "W1_status", "W2_status", "W3_status", "W4_status", "W5_status", "W6_status" ] } # # } End JSON 2018-04-03T00:00:00 2018 4 3 0 0 00 0.60 -1.20 387.0 2.70 0.72 0.40 2.25 0.63 2 2 2 2 2 2 2 2 1.30 1.30 -6 -1.20 -1.20 -1.20 -1.20 -1.20 -1.20 0.129 0.225 0.026 0.083 0.261 0.201 2 2 2 2 2 2 2018-04-03T01:00:00 2018 4 3 1 0 00 0.20 -1.50 387.0 2.90 0.77 0.46 2.64 0.74 2 2 2 2 2 2 2 2 1.30 1.30 -12 -1.50 -1.50 -1.50 -1.50 -1.50 -1.50 0.180 0.296 0.031 0.123 0.324 0.252 2 2 2 2 2 2 2018-04-03T02:00:00 2018 4 3 2 0 00 0.40 -1.50 383.0 2.90 0.76 0.54 2.89 0.84 2 2 2 2 2 2 2 2 1.30 1.30 -15 -1.50 -1.50 -1.50 -1.50 -1.50 -1.50 0.222 0.341 0.035 0.152 0.354 0.280 2 2 2 2 2 2 2018-04-03T03:00:00 2018 4 3 3 0 00 0.70 -2.30 383.0 3.50 0.90 0.91 3.70 1.20 2 2 2 2 2 2 2 2 2.00 1.39 -12 -2.30 -2.30 -2.30 -2.30 -2.30 -2.30 0.286 0.423 0.043 0.216 0.442 0.362 2 2 2 2 2 2 2018-04-03T04:00:00 2018 4 3 4 0 00 -0.50 -1.70 385.0 3.00 0.78 0.91 3.79 1.23 2 2 2 2 2 2 2 2 2.00 1.48 -6 -1.70 -1.70 -1.70 -1.70 -1.70 -1.70 0.321 0.446 0.050 0.238 0.442 0.372 2 2 2 2 2 2 2018-04-03T05:00:00 2018 4 3 5 0 00 -1.30 -1.60 385.0 2.40 0.63 0.75 3.17 0.85 2 2 2 2 2 2 2 2 2.00 1.57 -6 -1.60 -1.60 -1.60 -1.60 -1.60 -1.60 0.320 0.416 0.055 0.222 0.394 0.313 2 2 2 2 2 2 2018-04-03T06:00:00 2018 4 3 6 0 00 -2.10 0.00 383.0 2.30 0.60 0.50 1.41 0.33 2 2 2 2 2 2 2 2 1.00 1.53 -3 0.00 0.00 0.00 0.00 0.00 0.00 0.253 0.281 0.055 0.147 0.211 0.190 2 2 2 2 2 2 2018-04-03T07:00:00 2018 4 3 7 0 00 -1.40 1.40 374.0 2.10 0.52 0.15 0.00 0.00 2 2 2 2 2 2 2 2 1.00 1.49 -7 1.40 1.40 1.40 1.40 1.40 1.40 0.171 0.139 0.053 0.082 0.067 0.079 2 2 2 2 2 2 2018-04-03T08:00:00 2018 4 3 8 0 00 -0.30 1.00 369.0 2.30 0.56 0.02 0.00 0.00 2 2 2 2 2 2 2 2 1.00 1.44 -3 1.00 1.00 1.00 1.00 1.00 1.00 0.116 0.069 0.052 0.046 0.021 0.033 2 2 2 2 2 2 2018-04-03T09:00:00 2018 4 3 9 0 00 0.80 0.40 366.0 2.30 0.55 0.01 0.00 0.00 2 2 2 2 2 2 2 2 0.30 1.31 -1 0.40 0.40 0.40 0.40 0.40 0.40 0.079 0.034 0.050 0.026 0.007 0.014 2 2 2 2 2 2 2018-04-03T10:00:00 2018 4 3 10 0 00 2.00 0.00 374.0 2.10 0.52 0.15 0.00 0.00 2 2 2 2 2 2 2 2 0.30 1.18 -4 0.00 0.00 0.00 0.00 0.00 0.00 0.053 0.017 0.049 0.014 0.002 0.006 2 2 2 2 2 2 2018-04-03T11:00:00 2018 4 3 11 0 00 1.40 1.20 362.0 1.50 0.36 0.14 0.00 0.00 2 2 2 2 2 2 2 2 0.30 0.97 -1 1.20 1.20 1.20 1.20 1.20 1.20 0.036 0.008 0.047 0.008 0.001 0.002 2 2 2 2 2 2 2018-04-03T12:00:00 2018 4 3 12 0 00 1.80 1.50 360.0 1.40 0.33 0.07 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.72 -2 1.50 1.50 1.50 1.50 1.50 1.50 0.024 0.004 0.046 0.005 0.000 0.001 2 2 2 2 2 2 2018-04-03T13:00:00 2018 4 3 13 0 00 1.40 1.70 356.0 2.40 0.53 0.06 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.48 -2 1.70 1.70 1.70 1.70 1.70 1.70 0.017 0.002 0.044 0.003 0.000 0.000 2 2 2 2 2 2 2018-04-03T14:00:00 2018 4 3 14 0 00 1.20 1.70 352.0 2.70 0.60 0.03 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.35 -3 1.70 1.70 1.70 1.70 1.70 1.70 0.011 0.001 0.043 0.001 0.000 0.000 2 2 2 2 2 2 2018-04-03T15:00:00 2018 4 3 15 0 00 1.90 1.50 353.0 2.80 0.61 0.06 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.23 -5 1.50 1.50 1.50 1.50 1.50 1.50 0.008 0.001 0.042 0.001 0.000 0.000 2 2 2 2 2 2 2018-04-03T16:00:00 2018 4 3 16 0 00 2.60 1.40 356.0 2.60 0.58 0.17 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.11 -4 1.40 1.40 1.40 1.40 1.40 1.40 0.005 0.000 0.040 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T17:00:00 2018 4 3 17 0 00 2.80 1.50 355.0 2.60 0.57 0.26 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.07 -1 1.50 1.50 1.50 1.50 1.50 1.50 0.003 0.000 0.039 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T18:00:00 2018 4 3 18 0 00 2.00 1.40 343.0 2.50 0.52 0.19 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.04 2 1.40 1.40 1.40 1.40 1.40 1.40 0.002 0.000 0.038 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T19:00:00 2018 4 3 19 0 00 2.00 1.90 342.0 3.00 0.62 0.10 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.00 4 1.90 1.90 1.90 1.90 1.90 1.90 0.002 0.000 0.037 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T20:00:00 2018 4 3 20 0 00 2.10 1.90 343.0 3.20 0.66 0.10 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.00 5 1.90 1.90 1.90 1.90 1.90 1.90 0.001 0.000 0.036 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T21:00:00 2018 4 3 21 0 00 1.70 1.80 342.0 4.10 0.84 0.08 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.00 9 1.80 1.80 1.80 1.80 1.80 1.80 0.001 0.000 0.035 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T22:00:00 2018 4 3 22 0 00 3.20 2.30 347.0 5.20 1.07 0.17 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.00 9 2.30 2.30 2.30 2.30 2.30 2.30 0.000 0.000 0.033 0.000 0.000 0.000 2 2 2 2 2 2 2018-04-03T23:00:00 2018 4 3 23 0 00 3.10 2.00 343.0 5.70 1.14 0.29 0.00 0.00 2 2 2 2 2 2 2 2 0.00 0.00 7 2.00 2.00 2.00 2.00 2.00 2.00 0.000 0.000 0.032 0.000 0.000 0.000 2 2 2 2 2 2