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The Dynamics of Solar Flares and Magnetic Fields

Examining how coronal magnetic stability affects solar flare types.

― 6 min read


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Table of Contents

Solar flares are massive bursts of energy caused by the release of magnetic energy in the sun's atmosphere. This energy is stored in the coronal magnetic fields and released through a process known as magnetic reconnection. Sometimes, this release is accompanied by a Coronal Mass Ejection (CME), where plasma and magnetic fields escape into space. When this happens, we call it an eruptive flare. On the other hand, if no CME occurs, it is called a confined flare.

Solar flares and CMEs are different outcomes of the same physical processes that involve changes in the coronal fields. There are several reasons why solar eruptions happen, and researchers often categorize them into two types: driving mechanisms, which can produce an eruption, and trigger mechanisms, which ignite it. To completely have an eruption, the driving mechanism must take over after the trigger.

The pre-eruption magnetic configuration can primarily be represented in two models: the sheared arcade and the twisted flux rope. A sheared arcade has magnetic lines that extend and wind around the central axis. A twisted flux rope is more complex, with magnetic lines wrapping around a central axis above the polarity inversion line (PIL) and turning at least once.

For the twisted flux rope model, there is a radial force called the “hoop” force, arising from the interaction between the electric current and the self-generated magentic field. This hoop force pushes outward. Meanwhile, the external magnetic field applies a strapping force, which holds the rope down. If the strapping force decreases more quickly than the hoop force, the rope can become unstable, which is known as Torus Instability (TI).

TI is considered one of the main driving mechanisms for eruptions, along with flare reconnection. Researchers have looked into the stability of a toroidal current ring by considering only the hoop force and the strapping force. The decay index, a measure of how the external field changes with height, can reveal critical points where TI may trigger an eruption.

Recent studies have suggested that additional factors may also significantly affect the performance of the twisted flux rope. These findings have led to a more nuanced understanding of the critical decay index values that define when an eruption may occur. Analyzing data from numerous solar events has shown a range of behavior around these critical values.

Methods

This study examines the connection between the coronal magnetic field's stability and both confined and eruptive flares. To do this, we focus on the helicity ratio, which reflects the overall structure of magnetic fields, and the critical height for torus instability. By comparing these variables, we can better understand the factors contributing to different types of solar flares.

We analyzed magnetically active regions surrounding solar flares, focusing on a selection of ten flares that fall into the GOES class M1.0 or larger. Observations were made using 3D models of nonlinear force-free magnetic fields to determine the altitudes of these magnetic structures before the flares occurred.

The flare-relevant PIL was identified using magnetic field data obtained from the Solar Dynamics Observatory. The analysis involved two key steps: determining flaring polarity inversion lines and defining the spatial regions for stability analysis.

To investigate how the magnetic field and electric currents vary with height, we created models of magnetic field and electric current density. By applying statistical methods, we calculated the decay index, identifying critical heights associated with torus instability using different thresholds.

Results and Discussion

The results reveal some important findings about the relationship between the coronal magnetic field and solar flares. Notably, we discovered that the critical height for torus instability is often lower in eruptive flares compared to confined flares. This suggests that magnetic field configurations with a higher eruptive potential are also more likely to be unstable.

We observed that configurations leading to confined flares often had a higher critical height, indicating they were more robust than those associated with eruptive flares. This observation aligns with earlier studies that indicated lower coronal heights for eruptive events.

Interestingly, even though the mean values of critical heights for eruptive and confined events were distinct, the underlying altitudes of the current-weighted centers were not significantly different. This points to the idea that other aspects of the coronal magnetic field configuration may affect whether a flare erupts or remains confined.

The helicity ratio, which provides an overall measure of the magnetic field’s complexity, also plays a significant role. Our analysis showed that higher helicity ratios correlate with a greater likelihood of CME production, which further supports the relationship between magnetic field geometry and flare type.

Throughout our study, we identified that the predictions based on the NLFF modeling approach should be interpreted with caution. The altitudes derived from this modeling were often found to be limited, suggesting that a deeper understanding of coronal magnetic structures requires integrating various observational methods.

Given the differences in flare types and their correlation with the critical heights, we recommend further investigation into multiple factors affecting these events. This involves evaluating the methods used for measuring both helicity and stability, as well as validating model deductions through observational data.

Conclusion

In summary, the stability of the coronal magnetic field is crucial in determining whether solar flares will be confined or eruptive. By combining local measures like the critical height for torus instability with global measures like the helicity ratio, we have a clearer picture of how magnetic configurations affect flare outcomes.

Our findings highlight that configurations with a higher eruptive potential are more prone to instability, suggesting that particular characteristics of the coronal magnetic field are critical in predicting solar flare behavior. As we enhance our understanding in this area, the development of better models will help to forecast solar activities more accurately, potentially improving our ability to anticipate their impacts on space weather and the Earth's atmosphere.

Future studies should focus on a more extensive sample of events to confirm our results, allowing us to refine our understanding of these complex systems. Integration of various modeling techniques and observational approaches will enrich the current knowledge and lead to more robust predictions about solar flares and their related phenomena.

Original Source

Title: Stability of the coronal magnetic field around large confined and eruptive solar flares

Abstract: In order to improve our understanding on the pre-requisites of eruptive solar flares, we study and compare different measures that characterize the eruptive potential of solar active regions - the critical height for torus instability as a local measure and the helicity ratio as a global measure - with the structural properties of the underlying magnetic field, namely the altitude of the center of the current-carrying magnetic structure. Using time series of 3D optimization-based nonlinear force-free magnetic field models for 10 different active regions (ARs) around the time of large solar flares, we determine the altitudes of the current-weighted centers of the non-potential model structures. Based on the potential magnetic field, we inspect the decay index, $n$, in multiple vertical planes oriented along of or perpendicular to the flare-relevant polarity inversion line, and estimate the critical height ($h_{\mathrm{crit}}$) for torus instability (TI) using different thresholds of $n$. The critical heights are interpreted with respect to the altitudes of the current-weighted centers of the associated non-potential structures, as well as the eruptive character of the associated flares, and the eruptive potential of the host AR, as characterized by the helicity ratio. Our most important findings are that (i) $h_{\mathrm{crit}}$ is more segregated in terms of flare type than the helicity ratio, and that (ii) coronal field configurations with a higher eruptive potential (in terms of the helicity ratio) also appear to be more prone to TI. Furthermore, we find no pronounced differences in the altitudes of the non-potential structures prior to confined and eruptive flares.

Authors: Manu Gupta, J. K. Thalmann, A. M. Veronig

Last Update: 2024-02-19 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2402.12254

Source PDF: https://arxiv.org/pdf/2402.12254

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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