For a planet like the Earth, water plays a fundamental role in the global climate system. Today, the Earth is in radiative equilibrium balance where the insolation it receives from the Sun is balanced by outgoing infrared emission from the planet’s surface. This gives the Earth an average surface temperature of 288 K or 15 degrees Centigrade. If the Earth were closer to the Sun, it will receive a greater amount of insolation from the Sun and this will heat up the planet, causing more water vapour to be released into the atmosphere. The increase in atmospheric water vapour brings about a stronger greenhouse effect. This causes the Earth to give off more infrared radiation to balance the larger insolation it is getting from the Sun. As a result, if the Earth were nearer to the Sun, it will settle into a new radiative equilibrium balance with a somewhat higher mean surface temperature.
Nevertheless, there is a minimum distance a planet like the
Earth can be from its parent star before the amount of insolation received by
the planet becomes so great that radiative equilibrium balance can never be
achieved. Any closer than this minimum distance, the planet undergoes what is
known as a runaway greenhouse effect. As more water vapour is released into the
planet’s atmosphere, the greenhouse effect becomes stronger. This causes the
planet to become hotter and release yet more water vapour and so on.
Eventually, all water on the planet’s surface is vaporised and the surface
temperature everywhere on the planet settles at a scorching temperature of
~1400 K, rendering the planet uninhabitable for life. Due to the onset of runaway
greenhouse effect, the minimum distance a habitable Earth-like planet can be
from its parent star denotes the inner edge of the habitable zone around the
star. Any nearer, a runaway greenhouse effect occurs and makes the planet too
hot to be habitable.
Although a runaway greenhouse effect seems like a certainty
for an Earth-like planet that is too close to its parent star, it may not always
be the case since it assumes that there is a sufficient reservoir of water
everywhere on the planet’s surface. In fact, a planet whose surface is
predominately land with only small areas of surface water can escape a runaway
greenhouse effect entirely. A planet like this is referred to as a land planet.
In contrast, the Earth is commonly referred to as an ocean planet. On a land
planet, the rate at which water is delivered to the atmosphere is too slow to
trigger a runaway greenhouse effect. Water that evaporates from the hot regions
simply get transported and deposited in permanent cold traps on the planet. The
atmosphere of the land planet settles into a collapsed state with most of its
water inventory being captured in permanent cold traps. Potential permanent
cold traps include the planet’s night side or the planet’s poles. It is
important to note that the night side of a land planet can only serve as a cold
trap if the planet is tidally-locked where one hemisphere of the planet
constantly faces its parent star while the other hemisphere is in perpetual
night.
Figure 1: Artist’s impression of a desert planet with polar
ice caps.
Figure 2: Artist’s impression of a desert planet.
The cold trapping rate depends very much on the thickness of
the planet’s atmosphere. A thicker atmosphere will lead to less efficient cold
trapping as the permanent cold traps are warmer. The outcome is that a land
planet with an atmosphere that is not too thick can settle into a collapsed
state by accumulating most of its water inventory in permanent cold traps at a
rate that is sufficiently high to keep the planet from entering a runaway
greenhouse state. At these permanent cold traps, the low temperatures allow
water to accumulate as ice to form ice sheets. For a land planet that is not
tidally-locked and whose axial tilt is not too large, ice sheets can exist over
the poles. Similarly, a land planet that is tidally-locked can have ice sheets
on its permanent nightside hemisphere. The low temperatures at the permanent
cold traps suggest that all accumulated water is likely to be in the form of
solid ice. Nevertheless, it is worth considering if there are any processes
that can sustain bodies of liquid water for extended periods of time since
liquid water is an essential prerequisite for habitability.
As water accumulates as ice on an ice sheet, the ice sheet
thickens and gravity drives the flow of ice within the ice sheet. This has the
effect of transporting ice away from the cold traps, towards warmer regions
where the ice can potentially melt to produce liquid water. On Earth, ice
sheets that are just a couple of kilometres thick can transport ice over
distances of several hundred kilometres. As a result, one can imagine a land
planet with an ice sheet over one of its poles or over its nightside
hemisphere. Gravity driven ice flows bring the edge of the ice sheet towards
regions where the temperature is warm enough for melting to occur. This leads
to liquid water being present along the edge of the ice sheet, akin to pools of
melt water at the end of a glacier. Here, water evaporates and precipitates
back onto the ice sheet. In addition to liquid water at the edge of the ice
sheet, bodies of liquid water can also exist within the ice sheet itself if the
ice sheet happens to be over regions of sufficiently high geothermal heat flux.
Gliese 581c is a super-Earth orbiting the red dwarf star
Gliese 581. This exoplanet has at least 5.6 times the mass of Earth and it
orbits at the inner edge of the habitable zone around its parent star. The
close proximity to its parent star means that Gliese 581c is likely to be
tidally-locked, with a permanent nightside and a permanent dayside. Assuming
that Gliese 581c is a land planet with a small inventory of water and its
atmosphere is in a collapsed state where water is captured in permanent cold
traps, a simulation was preformed by Leconte et al. (2013) to determine its
properties. If Gliese 581c has a surface atmospheric pressure of 200 mbar, the
temperature on the permanent nightside hemisphere can be as low as -100 degrees
Centigrade. In contrast, the temperature on the planet’s permanent dayside can
get higher than 200 degrees Centigrade around the substellar point. Most of the
dayside hemisphere of Gliese 581c is simply a blistering hot desert.
Figure 3: Schematic diagram of Gliese 581c showing a dry
dayside hemisphere and an ice sheet over the nightside hemisphere. Credit: Leconte
et al. (2013)
A land planet with a limited water inventory can escape a
runaway greenhouse state and settle into a collapsed state with most of its
water being accumulated in ice sheets over its coldest regions. This is an
interesting scenario because such a planet can still remain somewhat habitable
even though it is closer to its parent star than the inner edge of the star’s
classical habitable zone. Thermal emission spectrum and reflection spectrum
from a planet can be used to differentiate whether the planet is in a runaway
greenhouse state or if the planet is in a collapsed state with most of its
water locked in ice sheets. If the planet is in a runaway greenhouse state, its
thermal emission spectrum will shift toward shorter wavelengths due to hotter
temperatures and its reflection spectrum will feature prominent water absorption
bands due to the large abundance of water vapour in the atmosphere. If the
planet is in a collapsed state where water is captured in permanent cold traps,
its thermal emission spectrum will shift toward longer wavelengths due to
cooler temperatures and its reflection spectrum will be more uniform due to the
low abundance of water vapour in the atmosphere.
Figure 4: Synthetic reflection spectrum (top) and thermal
emission spectrum (bottom) of Gliese 581c assuming the planet has a 200 mbar
atmosphere. The dash lines show the runaway greenhouse state while the solid
lines show the collapsed state. Credit: Leconte et al. (2013)
Reference:
Leconte et al. (2013), “3D climate modeling of close-in land
planets: Circulation patterns, climate moist bistability and habitability”, arXiv:1303.7079
[astro-ph.EP]