Numerical Simulation of Coronal Waves interacting with Coronal Holes: I. Basic Features
arXiv:1811.12073 · doi:10.3847/1538-4357/aa8cc9
Abstract
We developed a new numerical code that is able to perform 2.5D simulations of a magnetohydrodynamic (MHD) wave propagation in the corona, and its interaction with a low density region, such as a coronal hole (CH). We show that the impact of the wave on the CH leads to different effects, such as reflection and transmission of the incoming wave, stationary features at the CH boundary, or formation of a density depletion. We present a comprehensive analysis of the morphology and kinematics of primary and secondary waves, that is, we describe in detail the temporal evolution of density, magnetic field, plasma flow velocity, phase speed and position of the wave amplitude. Effects like reflection, refraction and transmission of the wave strongly support the theory that large scale disturbances in the corona are fast MHD waves and build the major distinction to the competing pseudo-wave theory. The formation of stationary bright fronts was one of the main reasons for the development of pseudo-waves. Here we show that stationary bright fronts can be produced by the interactions of an MHD wave with a CH. We find secondary waves that are traversing through the CH and we show that one part of these traversing waves leaves the CH again, while another part is being reflected at the CH boundary inside the CH. We observe a density depletion that is moving in the opposite direction of the primary wave propagation. We show that the primary wave pushes the CH boundary to the right, caused by the wave front exerting dynamic pressure on the CH.
References in corpus (16)
- First observations of a dome-shaped large-scale coronal EUV wave
- High cadence observations of a global coronal wave by EUVI/STEREO
- The Kinematics of a Globally Propagating Disturbance in the Solar Corona
- Numerical Simulation of an EUV Coronal Wave Based on the February 13, 2009 CME Event Observed by STEREO
- 'EUV Waves' are Waves: First Quadrature Observations of an EUV Wave from STEREO
- First SDO AIA Observations of a Global Coronal EUV "Wave": Multiple Components and "Ripples"
- First Evidence of Coexisting EIT Wave and Coronal Moreton Wave from SDO/AIA Observations
- Are "EIT Waves" Fast-Mode MHD Waves?
- Investigation of the Formation and Separation of An EUV Wave from the Expansion of A Coronal Mass Ejection
- Numerical Experiments of Wave-Like Phenomena Caused by the Disruption of an Unstable Magnetic Configuration
- What is the Nature of EUV Waves? First STEREO 3D Observations and Comparison with Theoretical Models
- Secondary Waves, and/or the "Reflection" From and "Transmission" Through a Coronal Hole of an EUV Wave Associated With the 2011 February 15 X2.2 Flare Observed With SDO/AIA and STEREO/EUVI
- Understanding the Physical Nature of Coronal "EIT Waves"
- Interaction of a Moreton/EIT wave and a coronal hole
- Can a Fast-mode EUV Wave Generate a Stationary Front?
- Formation of Coronal Shock Waves
Cited by in corpus (11)
- Impacts of EUV Wavefronts on Coronal Structures in Homologous Coronal Mass Ejections
- Total reflection of a flare-driven quasi-periodic EUV wave train at a coronal hole boundary
- Observations of Two Successive EUV Waves and their Mode Conversion
- Numerical Simulation of Coronal Waves Interacting with Coronal Holes: II. Dependence on Alfvén Speed Inside the Coronal Hole
- Numerical simulations of prominence oscillations triggered by external perturbations
- Radio evidence for a shock wave reflected by a coronal hole
- Numerical Simulation of Coronal Waves Interacting with Coronal Holes: III. Dependence on Initial Amplitude of the Incoming Wave
- Geometrical properties of the interaction between oblique incoming coronal waves and coronal holes
- Numerical study of solar eruption, extreme-ultraviolet wave propagation, and wave-induced prominence dynamics
- A new method for estimating global coronal wave properties from their interaction with solar coronal holes
- Investigation of the Two-Dimensional Velocity Field of the Large-Scale Coronal Wave from September 6, 2011 using the SOLERwave Tool