# Modelling atmospheric escape and MgII near-ultraviolet absorption of the   highly irradiated hot Jupiter WASP-12b

**Authors:** N. K. Dwivedi, M. L. Khodachenko, I. F. Shaikhislamov, L. Fossati, H., Lammer, Y. Sasunov, A. G. Berezutskiy, I. B. Miroshnichenko, K. G., Kislyakova, C. P. Johnstone, and M. G\"udel

arXiv: 1908.02527 · 2019-08-08

## TL;DR

This study models the upper atmosphere of hot Jupiter WASP-12b, including hydrogen chemistry and stellar wind interactions, to understand atmospheric escape and MgII ultraviolet absorption features.

## Contribution

It introduces a two-dimensional multi-fluid model that incorporates tidal forces, stellar wind effects, and XUV irradiation to simulate atmospheric escape and MgII absorption.

## Key findings

- Mass loss rate reaches 10^12 g/s controlled by stellar gravity.
- Tidal forces create dual streams of escaping material.
- MgII absorption matches observed ingress and egress timings.

## Abstract

We present two-dimensional multi-fluid numerical modelling of the upper atmosphere of the hot Jupiter WASP-12b. The model includes hydrogen chemistry, and self-consistently describes the expansion of the planetary upper atmosphere and mass loss due to intensive stellar irradiation, assuming a weakly magnetized planet. We simulate the planetary upper atmosphere and its interaction with the stellar wind (SW) with and without the inclusion of tidal force and consider different XUV irradiation conditions and SW parameters. With the inclusion of tidal force, even for a fast SW, the escaping planetary material forms two streams, propagating towards and away from the star. The atmospheric escape and related mass loss rate reaching the value of 10^12 gs^-1 appear to be mostly controlled by the stellar gravitational pull. We computed the column density and dynamics of MgII ions considering three different sets of SW parameters and XUV fluxes. The simulations enable to compute the absorption at the position of the Mg h line and to reproduce the times of ingress and egress. In case of a slow SW and without accounting for tidal force, the high orbital velocity leads to the formation of a shock approximately in the direction of the planetary orbital motion. In this case, mass loss is proportional to the stellar XUV flux. At the same time, ignoring of tidal effects for WASP-12b is a strong simplification, so the scenario with a shock, altogether is an unrealistic one.

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Source: https://tomesphere.com/paper/1908.02527