Figure 1: Artist’s impression of a habitable planet.
A previous study by Yang et al. (2013) showed that
tidally-locked terrestrial planets around red dwarf stars can remain habitable
at much closer distances to their host stars than previously thought due to a
stabilizing cloud feedback mechanism. Strong convection drives the formation of
water clouds that can cover most of the planet’s dayside, increasing the
planet’s reflectivity and keeping the planet cool. In a more recent study by
Yang et al. (2014), the focus shifts towards terrestrial planets around Sun-like
stars, especially those near the inner edge of the habitable zone (HZ). The
study examines the influence of planetary rotation on habitability.
A planet’s rotation rate determines its atmospheric
circulation by establishing the strength of the Coriolis effect and the length
of day. For a fast rotation rate, the Coriolis effect is strong and atmospheric
circulation is organised into latitudinal bands, like on Earth - Hadley cell,
Ferrel cell and Polar cell (Figure 2). Also, the short length of day due to
fast rotation results in small surface temperature differences between day and
night.
Figure 2: The three-cell model of atmospheric circulation on
Earth. From Equator to Pole - Hadley cell, Ferrel cell and Polar cell. Source:
Pearson Prentice Hall.
For a slow rotation rate, the Coriolis effect is weak and
the Hadley cells can extend globally. If the rotation rate is slow enough, the
dayside can become much warmer than the nightside, leading to atmospheric
circulation characterised by ascending air masses on the warm dayside and
descending air masses on the cold nightside.
Using 3D atmospheric general circulation models (GCMs), Yang
et al. (2014) examined, for an Earth-analogue, rotation periods ranging from 12
hours to 365 days. In the 3D GCMs, the stellar flux is increased until the mean
surface temperature reaches ~310 K, which is roughly when a runaway greenhouse
effect begins to occur and the planet becomes too hot for habitability.
Rotation rate determines the atmospheric circulation, which
in turn influences the spatial distribution of clouds on a planet. Clouds can
reflect a great deal of incoming stellar flux back into space. In doing so, clouds
play a vital role in regulating the planet’s surface temperature and hence, the
planet’s habitability. For example, greater cloud coverage increases the
planet’s reflectivity and keeps the planet cool.
The 3D GCMs revealed that for a given stellar flux, the
surface temperature of rapidly rotating planets is much higher than that of
slowly rotating planets. This is especially true for planets near the warm,
inner edge of the HZ. The Earth, considered a rapidly rotating planet in this
study, has high cloud coverage in the tropics due to the intertropical
convergence zone (ITCZ) associated with the ascending air masses of the Hadley
cells. These tropical clouds have the largest influence on Earth’s albedo (i.e.
Earth’s reflectivity) because the tropics receive the highest amount of stellar
flux.
If the stellar flux is increased for a rapidly rotating planet,
the equator-to-polar temperature gradient decreases, weakening the Hadley
cells, reducing tropical cloud coverage and decreases the planet’s albedo. The
end result is more warming of the planet. This drives a positive feedback where
the increase in stellar flux eventually leads to a runaway greenhouse effect,
creating temperatures too hot for habitability.
For slowly rotating planets, the atmospheric circulation
consists of Hadley cells that extend globally. This is unlike fast rotating
planets whose atmospheric circulation is organised into latitudinal bands. On a
slowly rotating planet, the substellar point (i.e. spot on the planet’s surface
where the planet’s host star is “directly overhead”) moves slowly across the
planet’s surface. Around the substellar point, convection leads to the
formation of clouds that can cover much of the planet’s dayside. These clouds
allow the planet to reflect incoming stellar flux, keeping the planet cool.
When stellar flux is increased for a slowly rotating planet,
convection becomes stronger due to more heating of the planet’s dayside. This
leads to the formation of yet more clouds, allowing the planet to reflect away
more incoming stellar flux and creates a negative feedback that stabilizes the
climate from overheating. As a result, the inner edge of the HZ for slowly
rotating planets can be much closer to the host star than for rapidly rotating
planets.
Figure 3: Dependence of planetary climate on rotation period
for planets orbiting a Sun-like star. (a) and (b): Global-mean surface
temperature (TS) and planetary albedo as a function of rotation period for a
given stellar flux. The surface heat capacity (D) is equivalent to 50m of
water. (c) and (d): Global-mean surface temperature (TS) and planetary albedo
as a function of stellar flux for a given rotation period with D of 50 m.
Source: Yang et al. (2014).
Figure 4: Differences in clouds and atmospheric circulation
between rapidly (left) and slowly (right) rotating planets. Source: Yang et al.
(2014).
Figure 5: Habitable zone boundaries as a function of stellar
type and planetary rotation rate for a 1D radiative-convective model and for
the 3D GCM. Blue line: outer edge of the HZ (Kopparapu et al. 2013); green
line: inner edge of the HZ (Kopparapu et al. 2013); black line: inner edge of
the habitable zone for rapidly rotating planets in this study; red line: inner
edge of the habitable zone for slowly rotating planets in this study (rotation
period of 128 days for G-type and F-type stars, and tidally-locked with an orbit
of 60 days for M-type and K-type stars); gray line: the tidal-locking radius.
Source: Yang et al. (2014).
Using the 3D GCMs, Yang et al. (2014) also examined a
Venus-analogue with Venus’ orbital characteristics, but with Earth’s atmosphere.
The results suggest that such a planet could be habitable, even though it
receives a higher stellar flux of 2610 W/m^2 versus 1360 W/m^2 that Earth gets
from the Sun. It would imply that when Venus went through a runaway greenhouse
to become the hellish, inhospitable place it now is, it must have had a higher
rotation rate at that time.
Figure 6: The climate of a planet with modern Earth’s
atmosphere and continental configuration, but in Venus’ orbit and with Venus’
(slow) rotation rate. (a): Time series of global-mean surface temperature (TS)
simulated for Venus’ rotation rate (slowly rotating, black), Earth’s rotation
rate (rapidly rotating, green) and Venus’ rotation rate with clouds
artificially set to zero (slowly rotating, no clouds, red). The planet quickly
tends toward a runaway greenhouse if it is rapidly rotating or has no clouds,
but is habitable if it is slowly rotating. (b): Global-mean TS and
vertically-integrated ocean temperature (Tocn) in a coupled ocean-atmosphere
simulation using Venus’ rotation rate. (c-e): maps of TS, planetary albedo and
thermal emission to space averaged over 1 day in the simulation. The black dot
in (c-e) is the transient substellar point, which moves eastward around the
planet with a period of 117 days. Source: Yang et al. (2014).
References:
- Yang et al. (2013), “Stabilizing Cloud Feedback
Dramatically Expands the Habitable Zone of Tidally Locked Planets”, arXiv:1307.0515
[astro-ph.EP]
- Yang et al. (2014), “Strong Dependence of the Inner Edge
of the Habitable Zone on Planetary Rotation Rate”, arXiv:1404.4992
[astro-ph.EP]
- Kopparapu et al. (2013), “Habitable Zones Around
Main-Sequence Stars: New Estimates”, arXiv:1301.6674 [astro-ph.EP]