the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
Global evolution of flux transfer events along the magnetopause from the dayside to the far tail
Abstract. Magnetic flux ropes are structures of magnetic field rolled-up along a longitudinal axis, which are forming in a variety of magnetised plasmas. In near-Earth space, flux ropes are a manifestation of energy transfer at the magnetopause and in the magnetotail current sheet. We present a new method to detect magnetic flux ropes in large-scale simulations, using only magnetic field line tracing. The method does not require prior identification of structures of interest such as current sheets or null lines, and thus allows one to identify flux ropes of any size and orientation, anywhere in the simulation domain. In this work, the new method is implemented in the hybrid-Vlasov model Vlasiator and demonstrated in global simulations of the terrestrial magnetosphere.
We study the evolution of flux ropes forming during flux transfer events on the dayside magnetopause under southward interplanetary magnetic field. It is found that flux ropes with an axial orientation along the dawn-dusk direction and propagating beyond the cusps will rapidly reconnect with the lobe magnetic field and vanish. In contrast, the flux ropes remaining near the equatorial plane and with an axial orientation along the flow direction, that is tangential to the magnetopause, can maintain their structure and propagate tens of Earth radii down the tail in the absence of a reconnecting shear magnetic field component. These results are a step forward in the global characterisation of flux ropes in and around the magnetosphere, and may help in guiding the search for elusive far-tail flux ropes in satellite measurements.
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Status: open (until 10 Feb 2025)
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RC1: 'Comment on angeo-2024-26', Anonymous Referee #1, 07 Jan 2025
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Summary:
This work presents a new method for identifying magnetic flux ropes from global simulation results. The advantages of this method is that it only requires the magnetic field information and does not require prior knowledge of existing structures like current sheets, reconnection lines, or the magnetopause surface. The authors outline the methodology and present an application with the hybrid Vlasov code Vlasiator.
The presentation of this work is very clear and provides a novel contribution to an important topic in space science. The identification of flux ropes in simulation is beneficial to the study of magnetospheric physics, solar physics, and any other space environment where magnetic reconnection occurs.
Overall, the methods, results and conclusions are well written. In particular, the methodology is both straightforward and appears quite effective at accomplishing the goal of flux rope identification. Additionally, the comparison with the topological identification of Alho et al. 2024 provides a meaningful point of validation that the dayside identified structures are indeed Flux Transfer Events.
Recommendation:
Below are detailed comments, my recommendation is to accept with minor revisions. Primarily, I think the authors could be more quantitative with the results that are presented. By providing more quantification the conclusions can be strengthened and this work will be easier to compare with future studies.
Detailed Comments:
Line 41: The authors use the term flux rope for both FTE and plasmoid, but what about Kelvin Helmholtz vorticies? They are not mentioned until the very last paragraph in the conclusions. If they are, or are not included in the ‘flux rope’ definition here it should be mentioned.
Figure1: Have you looked at the boundary points in terms of the points which fail only one of either R+ or R-? They would be the edges of the flux rope structure and might be regions of interest themselves.
Line 115: Why ‘significantly larger than the domain size’? I would assume if the traced point leaves the domain then surely the point is not flux rope.
Line 145: How is the fraction of omitted cells decided? Is it random, or geometric conditions set by the user?
Line 165: What radius are the field aligned currents coupled from? The data availability statement notes the large size of the output data, but it may beneficial to upload a simulation parameter input file ( or text file summarizing the simulation input parameters) for future comparisons.
Figure 2: This is where a quantified measure could be helpful. In the snapshot it’s clear there are more points identified with a larger Rcutoff, and at least one flux rope is missing between 3Rc and 7Rc. What I would like to see is what is the total flux rope volume for each of these panels? This could then be included in the video or even shown as a time series with a curve for each Rc setting. It could help justify the selection of Rcutoff = 7Rc.
Figure 4: The + and circles in panels e and f are difficult to distinguish between.
Line 245: With both the yellow circle O points and the green flux rope points, perhaps the coverage of the O points (within some distance threshold) could be reported here and used as validation. It could be reported as a percentage over time, again for the different choices of Rcutoff to show that 7Rc performs the best.
Figure 5: The satellite traces may show a better structure crossing if put into LMN coordinates.
Figure 6: I believe the X and Y scaling (horizontal axes) is different between some panels in the same column. This made it difficult to understand the point about the cross section shrinking. It would improve comparison between panels in a single column to have the scales the same.
Figure 7: Great use of perspective to summarize the flux rope detection results. Again, could be improved with an indication of how many flux ropes were found for each contour level. If identifying contiguous flux ropes is not currently possible, at least the total number of points (or volume of all points?).
Line 349: Figure 7 demonstrates that no dayside flux ropes survive to X=0, but is there a gradient or a sudden cutoff? If it is reconnection eroding the structure, maybe larger FTEs make it further downstream before vanishing?
Line 351: “any section of the flux rope presenting a magnetic field configuration anti-parallel to the lobe magnetic field will erode away due to magnetic reconnection.” Consider rewording slightly. The results only show a single flux rope that has its anti-parallel portion eroded, while every flux rope with such conditions could experience such erosion, it was not shown that this occurs in every instance. If the results do show this, then that should be included explicitly in the results section.
Line 356: Can it be estimated from these results what percentage of flux ropes are vanishing over the poles vs surviving downstream? Does it match some geometric ratio of the portion of the dayside X line length?
Line 377: Similar to above, it’s mentioned that ‘such a prediction would be perilous’. While I agree that a single simulation should not be over-extrapolated, the results can certainly be reported. How many low latitude flux ropes were found for this time interval? How does that compare to the number that vanished over the poles? The answer will be limited to this simulation setup, but nonetheless interesting.
Line 397: Does this imply that there may be holes that form in the field of flux rope points? Will this then make it more difficult to identify individual contiguous flux rope structures?
Line 449: How would this method tell the difference between a rolled up KH vortex and a low latitude flux rope which has been carried downstream?
Citation: https://doi.org/10.5194/angeo-2024-26-RC1
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