Steadiness of Coronal Heating
The EUI instrument on the Solar Orbiter spacecraft has obtained the most stable, high-resolution images of the solar corona from its orbit with a perihelion near 0.4 au. A sequence of 360 images obtained at 17.1 nm, between 2022 October 25 19:00 and 19:30 UT, is scrutinized. One image pixel correspo...
| Main Author: | |
|---|---|
| Format: | Article |
| Language: | English |
| Published: |
IOP Publishing
2023-01-01
|
| Series: | The Astrophysical Journal |
| Subjects: | |
| Online Access: | https://doi.org/10.3847/1538-4357/acf83a |
| _version_ | 1827786674383355904 |
|---|---|
| author | P. G. Judge |
| author_facet | P. G. Judge |
| author_sort | P. G. Judge |
| collection | DOAJ |
| description | The EUI instrument on the Solar Orbiter spacecraft has obtained the most stable, high-resolution images of the solar corona from its orbit with a perihelion near 0.4 au. A sequence of 360 images obtained at 17.1 nm, between 2022 October 25 19:00 and 19:30 UT, is scrutinized. One image pixel corresponds to 148 km at the solar surface. The widely held belief that the outer atmosphere of the Sun is in a continuous state of magnetic turmoil is pitted against the EUI data. The observed plasma variations appear to fall into two classes. By far the dominant behavior is a very low amplitude variation in brightness (1%) in the coronal loops, with larger variations in some footpoint regions. No hints of observable changes in magnetic topology are associated with such small variations. The larger-amplitude, more rapid, rarer, and less well organized changes are associated with flux emergence. It is suggested therefore that while magnetic reconnection drives the latter, most of the active corona is heated with no evidence of a role for large-scale (observable) reconnection. Since most coronal emission-line widths are subsonic, the bulk of coronal heating, if driven by reconnection, can only be of tangentially discontinuous magnetic fields, with angles below about 0.5 c _S / c _A ∼ 0.3 β , with β the plasma beta parameter (∼0.01) and c _S and c _A the sound and Alfvén speeds, respectively. If heated by multiple small flare-like events, then these must be ≲10 ^21 erg, i.e., picoflares. But processes other than reconnection have yet to be ruled out, such as viscous dissipation, which may contribute to the steady heating of coronal loops over active regions. |
| first_indexed | 2024-03-11T16:38:37Z |
| format | Article |
| id | doaj.art-d9d7caf1525c4ee39f0a48b57fbbef76 |
| institution | Directory Open Access Journal |
| issn | 1538-4357 |
| language | English |
| last_indexed | 2024-03-11T16:38:37Z |
| publishDate | 2023-01-01 |
| publisher | IOP Publishing |
| record_format | Article |
| series | The Astrophysical Journal |
| spelling | doaj.art-d9d7caf1525c4ee39f0a48b57fbbef762023-10-23T13:19:06ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-0195712510.3847/1538-4357/acf83aSteadiness of Coronal HeatingP. G. Judge0https://orcid.org/0000-0001-5174-0568High Altitude Observatory, National Center for Atmospheric Research , Boulder, CO 80307-3000, USAThe EUI instrument on the Solar Orbiter spacecraft has obtained the most stable, high-resolution images of the solar corona from its orbit with a perihelion near 0.4 au. A sequence of 360 images obtained at 17.1 nm, between 2022 October 25 19:00 and 19:30 UT, is scrutinized. One image pixel corresponds to 148 km at the solar surface. The widely held belief that the outer atmosphere of the Sun is in a continuous state of magnetic turmoil is pitted against the EUI data. The observed plasma variations appear to fall into two classes. By far the dominant behavior is a very low amplitude variation in brightness (1%) in the coronal loops, with larger variations in some footpoint regions. No hints of observable changes in magnetic topology are associated with such small variations. The larger-amplitude, more rapid, rarer, and less well organized changes are associated with flux emergence. It is suggested therefore that while magnetic reconnection drives the latter, most of the active corona is heated with no evidence of a role for large-scale (observable) reconnection. Since most coronal emission-line widths are subsonic, the bulk of coronal heating, if driven by reconnection, can only be of tangentially discontinuous magnetic fields, with angles below about 0.5 c _S / c _A ∼ 0.3 β , with β the plasma beta parameter (∼0.01) and c _S and c _A the sound and Alfvén speeds, respectively. If heated by multiple small flare-like events, then these must be ≲10 ^21 erg, i.e., picoflares. But processes other than reconnection have yet to be ruled out, such as viscous dissipation, which may contribute to the steady heating of coronal loops over active regions.https://doi.org/10.3847/1538-4357/acf83aActive sunSolar coronal heatingSolar coronal loops |
| spellingShingle | P. G. Judge Steadiness of Coronal Heating The Astrophysical Journal Active sun Solar coronal heating Solar coronal loops |
| title | Steadiness of Coronal Heating |
| title_full | Steadiness of Coronal Heating |
| title_fullStr | Steadiness of Coronal Heating |
| title_full_unstemmed | Steadiness of Coronal Heating |
| title_short | Steadiness of Coronal Heating |
| title_sort | steadiness of coronal heating |
| topic | Active sun Solar coronal heating Solar coronal loops |
| url | https://doi.org/10.3847/1538-4357/acf83a |
| work_keys_str_mv | AT pgjudge steadinessofcoronalheating |