Numerical simulations of ICME–ICME interactions

We present hydrodynamical simulations of the interaction of Coronal Mass Ejections (CME) in the Interplanetary Medium (IPM). In these events, two consecutive CMEs are launched from the Sun in similar directions within an interval of time of a few hours. In our numerical model, we assume that the amb...

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Main Authors: Niembro Tatiana, Lara Alejandro, González Ricardo Francisco, Cantó Jorge
Format: Article
Language:English
Published: EDP Sciences 2019-01-01
Series:Journal of Space Weather and Space Climate
Subjects:
Online Access:https://doi.org/10.1051/swsc/2018049
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author Niembro Tatiana
Lara Alejandro
González Ricardo Francisco
Cantó Jorge
author_facet Niembro Tatiana
Lara Alejandro
González Ricardo Francisco
Cantó Jorge
author_sort Niembro Tatiana
collection DOAJ
description We present hydrodynamical simulations of the interaction of Coronal Mass Ejections (CME) in the Interplanetary Medium (IPM). In these events, two consecutive CMEs are launched from the Sun in similar directions within an interval of time of a few hours. In our numerical model, we assume that the ambient solar wind is characterized by its velocity and mass-loss rate. Then, the CMEs are generated when the flow velocity and mass-loss rate suddenly change, with respect to the ambient solar wind conditions during two intervals of time, which correspond to the duration of each CME. After their interaction, a merged region is formed and evolve as a single structure into the IPM. In this work, we are interested in the general morphology of this merged region, which depends on the initial parameters of the ambient solar wind and the CMEs involved. In order to understand this morphology, we have performed a parametric study in which we characterize the effects of the initial parameters variations on the density and velocity profiles at 1 AU, using as reference the well-documented event of July 25th, 2004. Based on this parametrization we were able to reproduce the main features of the observed profiles ensuring the travel time and the speed and density magnitudes. Then, we apply the parametrization results to the interaction events of May 23, 2010; August 1, 2010; and November 9, 2012. With this approach and varying the values of the input parameters within the CME observational errors, our simulated profiles reproduce the main features observed at 1 AU. Even though we do not take into account the magnetic field, our models give a physical insight into the propagation and interaction of ICMEs.
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spelling doaj.art-01758bee65d547b79dfd36caf5665fa42022-12-21T22:04:55ZengEDP SciencesJournal of Space Weather and Space Climate2115-72512019-01-019A410.1051/swsc/2018049swsc170072Numerical simulations of ICME–ICME interactionsNiembro TatianaLara AlejandroGonzález Ricardo FranciscoCantó JorgeWe present hydrodynamical simulations of the interaction of Coronal Mass Ejections (CME) in the Interplanetary Medium (IPM). In these events, two consecutive CMEs are launched from the Sun in similar directions within an interval of time of a few hours. In our numerical model, we assume that the ambient solar wind is characterized by its velocity and mass-loss rate. Then, the CMEs are generated when the flow velocity and mass-loss rate suddenly change, with respect to the ambient solar wind conditions during two intervals of time, which correspond to the duration of each CME. After their interaction, a merged region is formed and evolve as a single structure into the IPM. In this work, we are interested in the general morphology of this merged region, which depends on the initial parameters of the ambient solar wind and the CMEs involved. In order to understand this morphology, we have performed a parametric study in which we characterize the effects of the initial parameters variations on the density and velocity profiles at 1 AU, using as reference the well-documented event of July 25th, 2004. Based on this parametrization we were able to reproduce the main features of the observed profiles ensuring the travel time and the speed and density magnitudes. Then, we apply the parametrization results to the interaction events of May 23, 2010; August 1, 2010; and November 9, 2012. With this approach and varying the values of the input parameters within the CME observational errors, our simulated profiles reproduce the main features observed at 1 AU. Even though we do not take into account the magnetic field, our models give a physical insight into the propagation and interaction of ICMEs.https://doi.org/10.1051/swsc/2018049Hydrodynamicsshock wavesSun: activitySun: coronal mass ejections (CMEs)solar wind
spellingShingle Niembro Tatiana
Lara Alejandro
González Ricardo Francisco
Cantó Jorge
Numerical simulations of ICME–ICME interactions
Journal of Space Weather and Space Climate
Hydrodynamics
shock waves
Sun: activity
Sun: coronal mass ejections (CMEs)
solar wind
title Numerical simulations of ICME–ICME interactions
title_full Numerical simulations of ICME–ICME interactions
title_fullStr Numerical simulations of ICME–ICME interactions
title_full_unstemmed Numerical simulations of ICME–ICME interactions
title_short Numerical simulations of ICME–ICME interactions
title_sort numerical simulations of icme icme interactions
topic Hydrodynamics
shock waves
Sun: activity
Sun: coronal mass ejections (CMEs)
solar wind
url https://doi.org/10.1051/swsc/2018049
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AT laraalejandro numericalsimulationsoficmeicmeinteractions
AT gonzalezricardofrancisco numericalsimulationsoficmeicmeinteractions
AT cantojorge numericalsimulationsoficmeicmeinteractions