Grand Tour of the Coronal Loops Model

  • Released Thursday, March 30, 2006
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This is a longer coronal loops tour combining components of the two previous versions (Animation IDs 3286 and 3287). The solar model is constructed from magnetogram data collected by SOHO/MDI. Because we do not see the full solar surface at any one time, the magnetograms collected over the course of a solar rotation are processed through a time-evolving solar surface model which provides a snapshot of the surface at a fixed time. The resulting magnetogram is then processed through the Potential Field Source Surface (PFSS) model which constructs the magnetic field above the solar surface. The magnetic field around the Sun is then analyzed for field lines, which creates the loop structures we see in the model. Hot plasma tends to flow along the magnetic field lines, creating the coronal loops. These loops are only visible at the higher temperatures corresponding to ultraviolet light, in this case, 195 angstroms, one of the filter wavelengths of SOHO/EIT. For this version, we color the coronal loops green for ready comparison to the EIT 195 angstrom imagery using the EIT standard color table.

We open with a time-series of EIT/195 Ångstrom images. The ultraviolet corona has been extended beyond the EIT image using a power-law falloff function fitted to the data.

We open with a time-series of EIT/195 Ångstrom images. The ultraviolet corona has been extended beyond the EIT image using a power-law falloff function fitted to the data.

We move closer to the surface of the model, near a small sunspot where we see the dipole structure of the field lines and spot region.

We move closer to the surface of the model, near a small sunspot where we see the dipole structure of the field lines and spot region.



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Please give credit for this item to:
NASA/Goddard Space Flight Center Scientific Visualization Studio

Release date

This page was originally published on Thursday, March 30, 2006.
This page was last updated on Wednesday, May 3, 2023 at 1:55 PM EDT.


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