2020
DOI: 10.3847/1538-4357/aba26b
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Inconsistencies Between Local and Global Measures of CME Radial Expansion as Revealed by Spacecraft Conjunctions

Abstract: The radial expansion of coronal mass ejections (CMEs) is known to occur from remote observations; from the variation of their properties with radial distance; and from local in situ plasma measurements showing a decreasing speed profile throughout the magnetic ejecta (ME). However, little is known on how local measurements compare to global measurements of expansion. Here, we present results from the analysis of 42 CMEs measured in the inner heliosphere by two spacecraft in radial conjunction.The magnetic fiel… Show more

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Cited by 34 publications
(72 citation statements)
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“…Image adapted from Vourlidas et al (2013), copyright by Springer and wide compared to solar cycle 23. Close to the Sun, the CME expansion is driven by the increased magnetic pressure inside the flux rope, while further out they most probably expand due to the decrease of the solar-wind dynamic pressure over distance (Lugaz et al 2020). Therefore, the increased width for CMEs of cycle 24 may be explained by the severe drop ( $ 50%) in the total (magnetic and plasma) heliospheric pressure (see e.g., McComas et al 2013;Gopalswamy et al 2014Gopalswamy et al , 2015Dagnew et al 2020a).…”
Section: General Characteristicsmentioning
confidence: 99%
“…Image adapted from Vourlidas et al (2013), copyright by Springer and wide compared to solar cycle 23. Close to the Sun, the CME expansion is driven by the increased magnetic pressure inside the flux rope, while further out they most probably expand due to the decrease of the solar-wind dynamic pressure over distance (Lugaz et al 2020). Therefore, the increased width for CMEs of cycle 24 may be explained by the severe drop ( $ 50%) in the total (magnetic and plasma) heliospheric pressure (see e.g., McComas et al 2013;Gopalswamy et al 2014Gopalswamy et al , 2015Dagnew et al 2020a).…”
Section: General Characteristicsmentioning
confidence: 99%
“…Another quantity that has been extensively investigated in previous studies is the scaling of the ICME magnetic field with heliocentric distance, which provides information on ICME global expansion (e.g. Démoulin & Dasso 2009;Lugaz et al 2020a). Estimates of the decay of the average magnetic field inside MEs range between −1.30 ± 0.09 and −1.95 ± 0.19 (e.g.…”
Section: Icme Magnetic Field Scaling With Heliocentric Distancementioning
confidence: 99%
“…Good et al 2019), whose properties can be investigated through numerous in situ fitting techniques (e.g. Al-Haddad et al 2013), and neglected non-flux rope configurations, which although more difficult to characterize, are nevertheless frequently observed at 1 au (Nieves-Chinchilla et al 2019) (for a notable exception, see Lugaz et al 2020a). As discussed in the following sections, complex magnetic configurations within ICMEs are in fact often the result of magnetic complexity changes attributable to the interaction of ICMEs with other solar wind structures, while classical FR structures are often a proxy for unperturbed propagation.…”
Section: Introductionmentioning
confidence: 99%
“…However, it might not be that simple, since the expansion rate of ICMEs inferred from in situ measurement is not necessarily a good indicator of the global expansion rate of the ICMEs. This was recently demonstrated by Lugaz et al (2020): by studying CMEs observed by spacecraft in conjunction but located at different radial distances from the Sun, they show that the global expansion rate of CMEs (obtained from measurements of multiple spacecraft) is not well correlated with the local measure of the expansion rate (calculated from in situ measurements by a single spacecraft). According to these authors, one scenario that could explain this discrepancy is that CMEs might expand faster close to the Sun (due to internal forces) than at 1 au (where the expansion is more controlled by external forces).…”
Section: Discussion and Physical Interpretationmentioning
confidence: 92%
“…ζ = 0.8), which could explain densities as low as 0.037 cm −3 . It is unfortunately not possible to know when and where the over-expansion of the ejecta started, or even if the expansion rate near the Sun was larger than at 1 au, as found by Lugaz et al (2020), but these simple calculations show that the very low density observed at 1 au on 2002 May 24 and 2002 May 25 could have been caused (completely or partially) by the over-expansion of ICME2.…”
Section: Discussion and Physical Interpretationmentioning
confidence: 94%