{"title":"Straight outta photosphere: Open solar flux without coronal modeling","authors":"Ismo Tähtinen, Timo Asikainen, Kalevi Mursula","doi":"arxiv-2408.11525","DOIUrl":null,"url":null,"abstract":"The open solar flux, that is, the total magnetic flux escaping the Sun, is\none of the most important parameters connecting solar activity to the Earth.\nThe open solar flux is commonly estimated from photospheric magnetic field\nmeasurements by making model assumptions about the solar corona. However, the\nquestion in which way the open solar flux is directly related to the\ndistribution of the photospheric magnetic field is still partly unknown. We aim\nto reconstruct the open solar flux directly from the photospheric magnetic\nfields without making any assumptions about the corona and without using\ncoronal hole observations, for instance. We modified an earlier vector sum\nmethod by taking magnetic field polarities into account and applied the method\nto the synoptic magnetograms of six instruments to determine the open solar\nflux from solar cycles 21-24. Results. The modified vector sum method produces\na vector of the global solar magnetic field whose magnitude closely matches the\nopen solar flux from the potential field source surface (PFSS) model both by\nthe absolute scale and the overall time evolution for each of the six\nmagnetograms. The latitude of this vector follows the Hale cycle by always\npointing toward the dominantly positive-polarity hemisphere, and its longitude\ncoincides with the location of the main coronal holes of the McIntosh Archive.\nWe find multi-year periods during which the longitude of the vector slowly\ndrifts or stays rather stationary in the Carrington frame. These periods are\npunctuated by times when the longitude moves rapidly in the Carrington frame.\nBy comparing the magnitude of this vector to the open solar flux calculated\nfrom the PFSS model with different source surface heights, we find that the\nbest match is produced with a source surface height $R_{ss} = 2.4 -\n2.5R_\\odot$.","PeriodicalId":501423,"journal":{"name":"arXiv - PHYS - Space Physics","volume":"108 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Space Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.11525","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The open solar flux, that is, the total magnetic flux escaping the Sun, is
one of the most important parameters connecting solar activity to the Earth.
The open solar flux is commonly estimated from photospheric magnetic field
measurements by making model assumptions about the solar corona. However, the
question in which way the open solar flux is directly related to the
distribution of the photospheric magnetic field is still partly unknown. We aim
to reconstruct the open solar flux directly from the photospheric magnetic
fields without making any assumptions about the corona and without using
coronal hole observations, for instance. We modified an earlier vector sum
method by taking magnetic field polarities into account and applied the method
to the synoptic magnetograms of six instruments to determine the open solar
flux from solar cycles 21-24. Results. The modified vector sum method produces
a vector of the global solar magnetic field whose magnitude closely matches the
open solar flux from the potential field source surface (PFSS) model both by
the absolute scale and the overall time evolution for each of the six
magnetograms. The latitude of this vector follows the Hale cycle by always
pointing toward the dominantly positive-polarity hemisphere, and its longitude
coincides with the location of the main coronal holes of the McIntosh Archive.
We find multi-year periods during which the longitude of the vector slowly
drifts or stays rather stationary in the Carrington frame. These periods are
punctuated by times when the longitude moves rapidly in the Carrington frame.
By comparing the magnitude of this vector to the open solar flux calculated
from the PFSS model with different source surface heights, we find that the
best match is produced with a source surface height $R_{ss} = 2.4 -
2.5R_\odot$.