{"format":"orbitwise.spaceweather.event","version":1,"id":"quiet_2024_03_17","kind":"quiet","title":"A quiet day, 17 March 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means of 1-minute OMNI data, time-shifted from the L1 spacecraft to Earth's bow shock nose (so the times are when the wind reached Earth, about 30 to 60 minutes after L1). Bz is the north-south field in GSM coordinates (negative = southward, which couples to Earth's field); Bt is the field strength. null = no 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average","meaning":"GOES XRS X-ray flux at Earth in W/m^2. long = 0.1-0.8 nm (XRS-B, the channel that sets the flare class: A < 1e-7 <= B < 1e-6 <= C < 1e-5 <= M < 1e-4 <= X). short = 0.05-0.4 nm (XRS-A). null = no good measurement (for example when the satellite was in Earth's shadow around the equinoxes).","satellite":"GOES-16","gaps_utc":[["2024-03-17T04:25:00Z","2024-03-17T05:52:00Z"]],"files":["sci_xrsf-l2-avg1m_g16_d20240317_v2-2-1.nc"],"source":"goes_xrs_ncei"}},"flare_list_min_class":"all","flares":[{"peak_unix":1710636120,"peak_utc":"2024-03-17T00:42:00Z","start_utc":"2024-03-17T00:31:00Z","end_utc":"2024-03-17T00:54:00Z","class":"C2.9","peak_w_m2":2.97e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710647940,"peak_utc":"2024-03-17T03:59:00Z","start_utc":"2024-03-17T03:53:00Z","end_utc":"2024-03-17T04:16:00Z","class":"C6.6","peak_w_m2":6.69e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710658320,"peak_utc":"2024-03-17T06:52:00Z","start_utc":"2024-03-17T06:45:00Z","end_utc":"2024-03-17T07:01:00Z","class":"C2.4","peak_w_m2":2.47e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710661260,"peak_utc":"2024-03-17T07:41:00Z","start_utc":"2024-03-17T07:33:00Z","end_utc":"2024-03-17T07:57:00Z","class":"C2.8","peak_w_m2":2.88e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710672180,"peak_utc":"2024-03-17T10:43:00Z","start_utc":"2024-03-17T10:35:00Z","end_utc":"2024-03-17T10:47:00Z","class":"C4.3","peak_w_m2":4.33e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710677580,"peak_utc":"2024-03-17T12:13:00Z","start_utc":"2024-03-17T12:03:00Z","end_utc":"2024-03-17T12:18:00Z","class":"C5.5","peak_w_m2":5.57e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710680340,"peak_utc":"2024-03-17T12:59:00Z","start_utc":"2024-03-17T12:55:00Z","end_utc":"2024-03-17T13:04:00Z","class":"C2.3","peak_w_m2":2.37e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710681780,"peak_utc":"2024-03-17T13:23:00Z","start_utc":"2024-03-17T13:11:00Z","end_utc":"2024-03-17T13:28:00Z","class":"C3.1","peak_w_m2":3.15e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710683040,"peak_utc":"2024-03-17T13:44:00Z","start_utc":"2024-03-17T13:36:00Z","end_utc":"2024-03-17T13:51:00Z","class":"C2.7","peak_w_m2":2.72e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710690180,"peak_utc":"2024-03-17T15:43:00Z","start_utc":"2024-03-17T15:27:00Z","end_utc":null,"class":"C4.9","peak_w_m2":4.95e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710691080,"peak_utc":"2024-03-17T15:58:00Z","start_utc":"2024-03-17T15:52:00Z","end_utc":"2024-03-17T16:11:00Z","class":"C3.3","peak_w_m2":3.35e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710704640,"peak_utc":"2024-03-17T19:44:00Z","start_utc":"2024-03-17T19:39:00Z","end_utc":"2024-03-17T19:53:00Z","class":"C2.6","peak_w_m2":2.61e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null},{"peak_unix":1710709920,"peak_utc":"2024-03-17T21:12:00Z","start_utc":"2024-03-17T20:54:00Z","end_utc":"2024-03-17T21:37:00Z","class":"C4.9","peak_w_m2":4.95e-06,"r_scale":0,"class_noaa_operational":null,"region":null,"location":null,"donki_id":null}],"cmes":[{"launch_unix":1710638700,"launch_utc":"2024-03-17T01:25:00Z","time21_5_utc":"2024-03-17T11:16:00Z","speed_km_s":353,"speed_range_km_s":null,"half_angle_deg":14,"direction_lat_deg":3,"direction_lon_deg":-90,"type":"S","source_location":null,"region":null,"linked_flare_ids":[],"earth_shock_utc":null,"earth_shock_ids":[],"linked_storm_ids":[],"donki_id":"2024-03-17T01:25:00-CME-001"},{"launch_unix":1710645120,"launch_utc":"2024-03-17T03:12:00Z","time21_5_utc":"2024-03-17T14:35:00Z","speed_km_s":325,"speed_range_km_s":[325,502],"half_angle_deg":45,"direction_lat_deg":-35,"direction_lon_deg":10,"type":"S","source_location":"S35W20","region":null,"linked_flare_ids":[],"earth_shock_utc":"2024-03-21T01:50:00Z","earth_shock_ids":["2024-03-21T01:50:00-IPS-001"],"linked_storm_ids":[],"donki_id":"2024-03-17T03:12:00-CME-001"},{"launch_unix":1710646560,"launch_utc":"2024-03-17T03:36:00Z","time21_5_utc":"2024-03-17T10:55:00Z","speed_km_s":499,"speed_range_km_s":[499,558],"half_angle_deg":31,"direction_lat_deg":-48,"direction_lon_deg":-24,"type":"S","source_location":"S35W20","region":null,"linked_flare_ids":[],"earth_shock_utc":"2024-03-21T01:50:00Z","earth_shock_ids":["2024-03-21T01:50:00-IPS-001"],"linked_storm_ids":[],"donki_id":"2024-03-17T03:36:00-CME-001"}],"shocks":[],"aurora":{"ovation":null,"ovation_note":"NOAA SWPC does not archive its OVATION Prime aurora forecasts, so past events use the Kp-driven oval model.","model":"starkov1994_kp","model_file":"res://assets/spaceweather/aurora_model.json","dipole_pole":{"lat":80.76,"lon":-72.75,"g10":-29358.4,"g11":-1416.8,"h11":4562.6,"epoch":2024.209,"model":"IGRF-14"}},"images":[],"notes":["The quietest day for Earth's magnetic field in 2024 and 2025 by the lowest daily sum of the definitive GFZ Kp index (Kp at or below 0+ all day; 7 January, 19 February and 26 December 2024 also stayed at 0+ or below).","It was near solar maximum, so the Sun still made small C-class flares: a quiet day for Earth is not a silent Sun."],"label":{"kind":"real_data"},"sources":[{"id":"gfz_kp","title":"Geomagnetic Kp index (definitive and nowcast), GFZ German Research Centre for Geosciences","credit":"Matzka, J., Bronkalla, O., Tornow, K., Elger, K. and Stolle, C. (2021): Geomagnetic Kp index. GFZ Data Services, doi:10.5880/Kp.0001","url":"https://kp.gfz.de/","licence":"CC BY 4.0"},{"id":"omni_hro_1min","title":"OMNI high-resolution 1-minute solar wind and magnetic field data, time-shifted to the Earth's bow shock nose (from ACE, Wind and DSCOVR)","credit":"J.H. King and N.E. Papitashvili, NASA/GSFC Space Physics Data Facility, OMNIWeb and CDAWeb","url":"https://omniweb.gsfc.nasa.gov/html/HROdocum.html","licence":"Public domain (NASA data, no copyright); acknowledge NASA/GSFC SPDF OMNIWeb"},{"id":"goes_xrs_ncei","title":"GOES-R XRS 1-minute average X-ray flux and flare summary, science-quality Level 2 (version 2-2-1)","credit":"NOAA National Centers for Environmental Information (NCEI), GOES-R Series XRS team","url":"https://www.ncei.noaa.gov/products/goes-r-extreme-ultraviolet-xray-irradiance","licence":"Public domain (US Government work, NOAA)"},{"id":"donki","title":"Space Weather Database Of Notifications, Knowledge, Information (DONKI): CMEs, flares, interplanetary shocks, storms","credit":"NASA Community Coordinated Modeling Center (CCMC) and the Moon to Mars Space Weather Analysis Office","url":"https://ccmc.gsfc.nasa.gov/DONKI/","licence":"Public domain (NASA data, no copyright); acknowledge NASA CCMC"},{"id":"igrf14","title":"International Geomagnetic Reference Field, 14th generation (IGRF-14), dipole terms g10, g11, h11","credit":"IAGA Working Group V-MOD (Alken et al., 2025); file from NOAA NCEI","url":"https://www.ngdc.noaa.gov/IAGA/vmod/igrf.html","licence":"Free use (IAGA reference model); cite IAGA V-MOD"},{"id":"starkov1994","title":"Auroral oval boundaries as a function of AL and Kp (Starkov 1994), coefficients as tabulated by Sigernes et al. (2011)","credit":"Starkov, G.V. (1994) Geomagnetism and Aeronomy 34(3), 331-336 and 34(1), 101-103; Sigernes, F. et al. (2011) Optica Pura y Aplicada 44(4), 599-603","url":"https://aurora.unis.no/doc/Sigernes_Oval.pdf","licence":"Published scientific coefficients (facts); our own code implements them"}]}