Abstract

Abstract The Sun is the primary source of energy for the Earth. The small changes in total solar irradiance (TSI) can affect our climate on the longer timescale. In the evolutionary timescale, the TSI varies by a large amount and hence its influence on the Earth’s mean surface temperature (T s ) also increases significantly. We develop a mass loss dependent analytical model of TSI in the evolutionary timescale and evaluated its influence on the T s . We determined the numerical solution of TSI for the next 8.23 Gyr to be used as an input to evaluate the T s which formulated based on a zero-dimensional energy balance model. We used the present-day albedo and bulk atmospheric emissivity of the Earth and Mars as initial and final boundary conditions, respectively. We found that the TSI increases by 10% in 1.42 Gyr, by 40% in about 3.4 Gyr, and by 120% in about 5.229 Gyr from now, while the T s shows an insignificant change in 1.644 Gyr and increases to 298.86 K in about 3.4 Gyr. The T s attains the peak value of 2319.2 K as the Sun evolves to the red giant and emits the enormous TSI of 7.93 × 106 W m−2 in 7.676 Gys. At this temperature Earth likely evolves to be a liquid planet. In our finding, the absorbed and emitted flux equally increases and approaches the surface flux in the main sequence, and they are nearly equal beyond the main sequence, while the flux absorbed by the cloud shows the opposite trend.

Highlights

  • The total solar irradiance (TSI) varies by a large amount and its influence on the Earth’s mean surface temperature (Ts) increases significantly

  • We determined the numerical solution of TSI for the 8.23 Gyrs to be used as an input to evaluate the Ts which formulated based on a zero-dimensional energy balance model

  • We found that the TSI increases by 10% in 1.42 Gyr, by 40% in about 3.4 Gyrs, and by 120% in about 5.229 Gyrs while the Ts shows an insignificant change in 1.644 Gyrs and increases to 298.86 K in about 3.4 Gyrs

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Summary

INTRODUCTION

The Sun is the largest energy source to the Earth’s atmosphere (Kren 2015; Kren et al, 2017). It is varying with time and its tiny changes in TSI affect the Earth’s climate in the longer timescale (Eddy 1976) This idea is strengthened by many other studies (Haigh 2007; Lean & Rind 2008; Gray et al, 2010; Ineson 2011; Ermolli et al, 2013; Solanki et al, 2013; Kopp 2016). O’Malley-James (2013) used time-dependent luminosity to study the TSI variability and found its influence on Ts in the evolutionary timescale. Shukure et al (2021, submitted to APJ) They developed a mass-loss dependent solar luminosity in the evolutionary timescale. They calculate the mass-loss at each interval of 1 million years by subtracting every newly reduced solar mass from the present-day solar mass Following this method, we calculate the mass-loss to model TSI in the evolutionary timescale. We used the numerical method to solve the newly formulated models by setting some boundary conditions to ε and α that will be explained in detail in the method part

The Solar Mass-loss
Luminosity-mass Loss Relation
Modeling
Earth’s Mean Surface Temperature Variation
Numerical Computations of the Model
Total solar irradiance variability in the evolutionary timescale
Earth’s Mean Surface Temperature Variation in Evolutionary Timescale
Variation beyond the main sequence
Findings
CONCLUSION
Full Text
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