Abstract

Aims. Our goal is to constrain models of active region formation by tracking the average motion of active region polarity pairs as they emerge onto the surface. Methods. We measured the motion of the two main opposite polarities in 153 emerging active regions using line-of-sight magnetic field observations from the Solar Dynamics Observatory Helioseismic Emerging Active Region (SDO/HEAR) survey. We first measured the position of each of the polarities eight hours after emergence, when they could be clearly identified, using a feature recognition method. We then tracked their location forwards and backwards in time. Results. We find that, on average, the polarities emerge with an east-west orientation and the separation speed between the polarities increases. At about 0.1 days after emergence, the average separation speed reaches a peak value of 229 ± 11 ms−1, and then starts to decrease. About 2.5 days after emergence the polarities stop separating. We also find that the separation and the separation speed in the east-west direction are systematically larger for active regions that have higher flux. The scatter in the location of the polarities increases from about 5 Mm at the time of emergence to about 15 Mm at two days after emergence. Conclusions. Our results reveal two phases of the emergence process defined by the rate of change of the separation speed as the polarities move apart. Phase 1 begins when the opposite polarity pairs first appear at the surface, with an east-west alignment and an increasing separation speed. We define Phase 2 to begin when the separation speed starts to decrease, and ends when the polarities have stopped separating. This is consistent with a previous study: the peak of a flux tube breaks through the surface during Phase 1. During Phase 2 the magnetic field lines are straightened by magnetic tension, so that the polarities continue to move apart, until they eventually lie directly above their anchored subsurface footpoints. The scatter in the location of the polarities is consistent with the length and timescales of supergranulation, supporting the idea that convection buffets the polarities as they separate.

Highlights

  • Solar activity is driven by magnetic fields resulting from a dynamo operating inside the Sun

  • We measured the motion of the two main opposite polarities in 153 emerging active regions using line-of-sight magnetic field observations from the Solar Dynamics Observatory Helioseismic Emerging Active Region (SDO/HEAR) survey

  • This is consistent with an east-west oriented flux tube rising through the surface: the separation speed is fastest as the apex of the tube breaks the surface, the polarities slow down to reach a null separation speed once they are above their anchoring depths (e.g. Chen et al 2017)

Read more

Summary

Introduction

Solar activity is driven by magnetic fields resulting from a dynamo operating inside the Sun. Simple active regions consist of a pair of opposite polarities that grow in size and magnetic flux, separate, and develop a tilt angle (for a summary of observed properties see van Driel-Gesztelyi & Green 2015). They have typical lifetimes of days (lower flux regions) to weeks (higher flux regions). High-cadence, full-disc observation monitoring campaigns such as the Michelson Doppler Imager onboard the Solar and Heliospheric Observatory (SOHO/MDI; Scherrer et al 1995) and the Helioseismic and Magnetic Imager onboard the Solar Dynamics Observatory (SDO/HMI; Scherrer et al 2012) have provided a wealth of data These observations make it possible to perform statistical analyses that trace the evolution of active regions with higher and spatial and temporal resolution

Measuring the location of the magnetic polarities
Motion of the individual magnetic polarities
Phases of emergence
Scatter in the motion of the magnetic polarities
Findings
Summary
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call