Abstract

We present a new computational approach that addresses the difficulty of obtaining the correct interaction between the solar corona and the transition region in response to rapid heating events. In the coupled corona, transition region and chromosphere system, an enhanced downward conductive flux results in an upflow (chromospheric evaporation). However, obtaining the correct upflow generally requires high spatial resolution in order to resolve the transition region. With an unresolved transition region, artificially low coronal densities are obtained because the downward heat flux jumps across the unresolved region to the chromosphere, underestimating the upflows. Here, we treat the lower transition region as a discontinuity that responds to changing coronal conditions through the imposition of a jump condition that is derived from an integrated form of energy conservation. To illustrate and benchmark this approach against a fully resolved one-dimensional model, we present field-aligned simulations of coronal loops in response to a range of impulsive (spatially uniform) heating events. We show that our approach leads to a significant improvement in the coronal density evolution than just when using coarse spatial resolutions insufficient to resolve the lower transition region. Our approach compensates for the jumping of the heat flux by imposing a velocity correction that ensures that the energy from the heat flux goes into driving the transition region dynamics, rather than being lost through radiation. Hence, it is possible to obtain improved coronal densities. The advantages of using this approach in both one-dimensional hydrodynamic and three-dimensional magnetohydrodynamic simulations are discussed.

Highlights

  • The interaction between the solar corona and chromosphere is central to understanding the observed properties of magnetically closed coronal loops

  • The purpose of this paper is to present a physically motivated approach to deal with this problem by using an integrated form of energy conservation that treats the unresolved region of the lower transition region (TR) as a discontinuity, that responds to changing coronal conditions through the imposition of a jump condition

  • The effectiveness of the unresolved transition region (UTR) jump condition to obtain a physically realistic evolution, through the complete coronal heating and cooling cycle, when employed with coarse resolution is investigated for a series of impulsive coronal heating events

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Summary

Introduction

The interaction between the solar corona and chromosphere is central to understanding the observed properties of magnetically closed coronal loops. It is well known that if the corona is heated impulsively (by for example, a flare, microflare or nanoflare), both the temperature and density increase and decline, with the time of peak temperature preceding that of the peak density. The changes in density can only be accounted for by mass exchange between the corona and chromosphere, mediated by the transition region (TR). Recognising the role of the TR is essential for developing reliable models of impulsive heating. For a static equilibrium loop with steady heating, the TR is defined as the region extending from the top of the chromosphere to the location where thermal conduction changes from an energy loss to a gain The energy balance in the TR is approximately between downward thermal conduction and optically thin radiation (for a loop in thermal equilibrium)

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