Abstract

Abstract. The residence time of energy in a planetary atmosphere, τ, which was recently introduced and computed for the Earth's atmosphere (Osácar et al., 2020), is here extended to the atmospheres of Venus, Mars and Titan. τ is the timescale for the energy transport across the atmosphere. In the cases of Venus, Mars and Titan, these computations are lower bounds due to a lack of some energy data. If the analogy between τ and the solar Kelvin–Helmholtz scale is assumed, then τ would also be the time the atmosphere needs to return to equilibrium after a global thermal perturbation.

Highlights

  • When the inflow, Fi, of any substance into a box is equal to the outflow, Fo, the amount of that substance in the box, M, is constant

  • In this work we extend the substance that flows in the box from matter to energy, and the residence time is where E is the total energy in the box, and F is the energy flux that enters or leaves it

  • In Stix (2003) it is shown that the Kelvin– Helmholtz timescale (KH) corresponds to both the time that a photon takes from the core until it leaves the surface and the time necessary for the star to return to equilibrium after a global perturbation

Read more

Summary

Introduction

Fi, of any substance into a box is equal to the outflow, Fo, the amount of that substance in the box, M, is constant. This constitutes an equilibrium or steady state. Planetary atmospheres constitute steady-state problems, because the storage of energy in their interior is not systematically increasing or decreasing. Several authors have previously considered the energy–residence-time relation in other types of problems (Mcilveen, 1992, 2010; Harte, 1988). The structure of this communication is the following: Sect.

Forms of energy in a planetary atmosphere
Residence time of energy in the Sun
Findings
Discussion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call