Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape

We examine the transition from diffusion-limited to drag-off escape using a direct simulation Monte Carlo (DSMC) model developed to simulate planetary atmospheres, referred to as Harrah. A 1D spherically symmetric DSMC model is used to simulate two-component atmospheres to focus on the impact of rar...

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Main Authors: Jack C. Evans, Shane Robert Carberry Mogan, Robert E. Johnson, Orenthal J. Tucker
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Planetary Science Journal
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Online Access:https://doi.org/10.3847/PSJ/ada369
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author Jack C. Evans
Shane Robert Carberry Mogan
Robert E. Johnson
Orenthal J. Tucker
author_facet Jack C. Evans
Shane Robert Carberry Mogan
Robert E. Johnson
Orenthal J. Tucker
author_sort Jack C. Evans
collection DOAJ
description We examine the transition from diffusion-limited to drag-off escape using a direct simulation Monte Carlo (DSMC) model developed to simulate planetary atmospheres, referred to as Harrah. A 1D spherically symmetric DSMC model is used to simulate two-component atmospheres to focus on the impact of rarefaction on thermal diffusion. The results for the escape rates and thermal structure are characterized using a mass-averaged Jeans parameter, λ _avg,0 , and Knudsen number, Kn _a,0 , defined at a reference radial distance r _0 . As a test of the model, we simulated the escape of N _2 and H _2 self-consistently for conditions of Pluto’s upper atmosphere observed during the New Horizons mission. As expected, the DSMC result for H _2 escape is consistent with the diffusion-limited approximation, and H _2 escape has little effect on the background N _2 atmosphere. Then we examined the transition from diffusion-limited to drag-off escape for two-component atmospheres characterized by mass-averaged Knudsen numbers and Jeans parameters of Kn _a,0  ≈ 0.01–0.1 and λ _avg,0  ≈ 0.5–13, respectively. We found that escape transitioned from hydrodynamic escape to an enhanced Jeans-like escape at λ _avg,0  ≈ 3.0–3.6. For values of λ _avg,0  < 3.0–3.6, escape was hydrodynamic and in the blow-off regime. For values of λ _avg,0  >≈ 3.6, the DSMC results indicated that using the diffusion-limited and drag-off approximations can lead to inaccurate estimates of the escape rate.
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spelling doaj-art-e5e0fcf3ca444116bc6dcd054e5e188e2025-02-06T07:03:42ZengIOP PublishingThe Planetary Science Journal2632-33382025-01-01623910.3847/PSJ/ada369Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off EscapeJack C. Evans0Shane Robert Carberry Mogan1https://orcid.org/0000-0002-0261-8117Robert E. Johnson2https://orcid.org/0000-0001-7798-5918Orenthal J. Tucker3https://orcid.org/0000-0002-8235-5440Stanford University , Stanford, CA, USASpace Sciences Laboratory , University of California, Berkeley, CA, USAUniversity of Virginia , Charlottesville, VA, USANASA Goddard Space Flight Center , Greenbelt, MD, USAWe examine the transition from diffusion-limited to drag-off escape using a direct simulation Monte Carlo (DSMC) model developed to simulate planetary atmospheres, referred to as Harrah. A 1D spherically symmetric DSMC model is used to simulate two-component atmospheres to focus on the impact of rarefaction on thermal diffusion. The results for the escape rates and thermal structure are characterized using a mass-averaged Jeans parameter, λ _avg,0 , and Knudsen number, Kn _a,0 , defined at a reference radial distance r _0 . As a test of the model, we simulated the escape of N _2 and H _2 self-consistently for conditions of Pluto’s upper atmosphere observed during the New Horizons mission. As expected, the DSMC result for H _2 escape is consistent with the diffusion-limited approximation, and H _2 escape has little effect on the background N _2 atmosphere. Then we examined the transition from diffusion-limited to drag-off escape for two-component atmospheres characterized by mass-averaged Knudsen numbers and Jeans parameters of Kn _a,0  ≈ 0.01–0.1 and λ _avg,0  ≈ 0.5–13, respectively. We found that escape transitioned from hydrodynamic escape to an enhanced Jeans-like escape at λ _avg,0  ≈ 3.0–3.6. For values of λ _avg,0  < 3.0–3.6, escape was hydrodynamic and in the blow-off regime. For values of λ _avg,0  >≈ 3.6, the DSMC results indicated that using the diffusion-limited and drag-off approximations can lead to inaccurate estimates of the escape rate.https://doi.org/10.3847/PSJ/ada369Atmospheric evolutionExospherePluto
spellingShingle Jack C. Evans
Shane Robert Carberry Mogan
Robert E. Johnson
Orenthal J. Tucker
Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
The Planetary Science Journal
Atmospheric evolution
Exosphere
Pluto
title Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
title_full Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
title_fullStr Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
title_full_unstemmed Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
title_short Thermally Driven Atmospheric Escape: Transition from Diffusion-limited to Drag-off Escape
title_sort thermally driven atmospheric escape transition from diffusion limited to drag off escape
topic Atmospheric evolution
Exosphere
Pluto
url https://doi.org/10.3847/PSJ/ada369
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