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Solar Magnetic Carpet III: Coronal Modelling of Synthetic Magnetograms

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Abstract

This article is the third in a series working towards the construction of a realistic, evolving, non-linear force-free coronal-field model for the solar magnetic carpet. Here, we present preliminary results of 3D time-dependent simulations of the small-scale coronal field of the magnetic carpet. Four simulations are considered, each with the same evolving photospheric boundary condition: a 48-hour time series of synthetic magnetograms produced from the model of Meyer et al. (Solar Phys. 272, 29, 2011). Three simulations include a uniform, overlying coronal magnetic field of differing strength, the fourth simulation includes no overlying field. The build-up, storage, and dissipation of magnetic energy within the simulations is studied. In particular, we study their dependence upon the evolution of the photospheric magnetic field and the strength of the overlying coronal field. We also consider where energy is stored and dissipated within the coronal field. The free magnetic energy built up is found to be more than sufficient to power small-scale, transient phenomena such as nanoflares and X-ray bright points, with the bulk of the free energy found to be stored low down, between 0.5 – 0.8 Mm. The energy dissipated is currently found to be too small to account for the heating of the entire quiet-Sun corona. However, the form and location of energy-dissipation regions qualitatively agree with what is observed on small scales on the Sun. Future MHD modelling using the same synthetic magnetograms may lead to a higher energy release.

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Acknowledgements

KAM and DHM gratefully acknowledge the support of the Leverhulme Trust and the STFC. DHM would like to thank the Royal Society for their support through the Research Grant Scheme. DHM and CEP acknowledge support from the EU under FP7.

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Correspondence to K. A. Meyer.

Electronic Supplementary Material

Below are the links to the electronic supplementary material.

magnet48_bz_2hr.mpg (18.7 MB)

magnet48b_free_ht.mpg (1.9 MB)

magnet48b_free_xy_bz.mpg (5.9 MB)

magnet48b_free_xz.mpg (882 kB)

magnet48b_j_xy_bz.mpg (7.4 MB)

magnet48b_q_ht.mpg (1.7 MB)

magnet48b_q_xy_3_10.mpg (2.2 MB)

magnet48b_q_xy_bz.mpg (7.3 MB)

magnet48b_q_xz.mpg (878 kB)

magnet48b_q_xz_log.mpg (930 kB)

Appendix: Images from Movies

Appendix: Images from Movies

This appendix contains four figures, each with six images spaced one hour apart from t=144 hours to t=149 hours, taken from some of the xy-plane movies included with this article.

Figure 8
figure 8

Free magnetic-energy density integrated along the line-of-sight for the three-gauss overlying field simulation. The images are shown in the xy-plane saturated at ± 1.9×1022 ergs. Contours of B z at z=0 Mm are over-plotted where red contours represent the positive magnetic field and green contours represent the negative field at levels of ± [7,13,27,53,106] gauss. The images are shown at (a) t=144 hours, (b) t=145 hours, (c) t=146 hours, (d) t=147 hours, (e) t=148 hours, and (f) t=149 hours. An animation of this figure is available in the online journal.

Figure 9
figure 9

Normalised j 2 integrated in z, shown in the xy-plane, for the three-gauss overlying field simulation. Darker regions correspond to higher values. Contours of B z at z=0 Mm are over-plotted where red contours represent the positive magnetic field and green contours represent the negative field at levels of ± [7,13,27,53,106] gauss. The images are shown at (a) t=144 hours, (b) t=145 hours, (c) t=146 hours, (d) t=147 hours, (e) t=148 hours, and (f) t=149 hours. An animation of this figure is available in the online journal.

Figure 10
figure 10

Rate of energy dissipation [Q] integrated along the line-of-sight, for the three-gauss overlying field simulation. The images are shown in the xy-plane saturated at 1.5×105 ergs cm−2 s−1. Darker regions correspond to higher values. Contours of B z at z=0 Mm are over-plotted, where red contours represent the positive magnetic field and green contours represent the negative field at levels of ± [7,13,27,53,106] gauss. The images are shown at (a) t=144 hours, (b) t=145 hours, (c) t=146 hours, (d) t=147 hours, (e) t=148 hours, and (f) t=149 hours. An animation of this figure is available in the online journal.

Figure 11
figure 11

Rate of energy dissipation [Q] for the three-gauss overlying field simulation. The images are shown in the xy-plane at z=3 Mm, saturated at 810 ergs cm−2 s−1. Darker regions correspond to higher values. They are shown at (a) t=144 hours, (b) t=145 hours, (c) t=146 hours, (d) t=147 hours, (e) t=148 hours, and (f) t=149 hours. An animation of this figure is available in the online journal.

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Meyer, K.A., Mackay, D.H., van Ballegooijen, A.A. et al. Solar Magnetic Carpet III: Coronal Modelling of Synthetic Magnetograms. Sol Phys 286, 357–384 (2013). https://doi.org/10.1007/s11207-013-0272-1

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  • DOI: https://doi.org/10.1007/s11207-013-0272-1

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