Dust in brown dwarfs and extra-solar planets. VII. Cloud formation in diffusive atmospheres

TL;DR

This paper introduces a new cloud formation model for brown dwarf and exoplanet atmospheres that incorporates turbulent mixing and diffusion, revealing complex cloud structures and non-solar element ratios.

Contribution

The model combines cloud particle moment method with diffusive mixing, providing a more realistic simulation of cloud formation and element distribution in atmospheres.

Findings

Fewer but larger cloud particles in hot Jupiter models.

Steep decline of condensable elements above cloud base.

Formation of a second Na2S cloud layer in cooler atmospheres.

Abstract

The precipitation of cloud particles in brown dwarf and exoplanet atmospheres establishes an ongoing downward flux of condensable elements. To understand the efficiency of cloud formation, it is therefore crucial to quantify the replenishment mechanism that is able to compensate for the element losses in the upper atmosphere, to keep the extrasolar weather cycle running. In this paper, we introduce a new cloud formation model by combining the cloud particle moment method of Helling & Woitke with a diffusive mixing approach, taking into account turbulent mixing and gas-kinetic diffusion for both gas and cloud particles. The equations are of diffusion-reaction type and are solved time-dependently for a prescribed 1D atmospheric structure, until the model has relaxed toward a time-independent solution. In comparison to our previous models, the new hot Jupiter model results (Teff=2000K, log g=3) show fewer but larger cloud particles which are more concentrated towards the cloud base. The abundances of condensable elements in the gas phase are featured by a steep decline above the cloud base, followed by a shallower, monotonous decrease towards a plateau, the level of which depends on temperature. The chemical composition of the cloud particles also differs significantly from our previous models. Due to the condensation of specific condensates like Mg2SiO4[s] in deeper layers, certain elements, such as Mg, are almost entirely removed from the gas phase early. This leads to unusual (and non-solar) element ratios in higher atmospheric layers, which then favours the formation of SiO[s] and SiO2[s], for example, rather than MgSiO3[s]. Such condensates are not expected in phase-equilibrium models that start from solar abundances. Above the main silicate cloud layer, which is enriched with iron and metal oxides, we find a second cloud layer made of Na2S[s] particles in cooler models (Teff<1500K).