Hot air balloons over Malqata, Egypt, site of the jubilee palace of Amenhotep III (ca. 1350 BC)
Recent work by Eric Lopez and Jonathan Fortney brings welcome clarity to the bewildering array of Kepler transit data on small planets. These esteemed planetologists just circulated a preprint entitled “Understanding the mass-radius relation for sub-Neptunes: Radius as a proxy for composition” (hereafter LF13). It addresses questions that have surfaced several times in this blog: How can we distinguish Super Earths from Neptune-like exoplanets? And what is the likely composition of each species? That topic is explored here, here, here, here, and most recently here.
puff threshold
Using the results from a large ensemble of thermal evolution
models, LF13 draw a physically motivated boundary between true Super Earths (which
are scaled-up versions of Earth, consisting only of heavy elements) and planets
like Uranus and Neptune (which maintain at least a small percentage of their
mass in a hydrogen/helium (H/He) envelope).
As Lopez and Fortney conclude, “for most of Kepler’s Neptune and sub-Neptune
sized planets, radius is quite independent of planet mass and is instead a
direct measure of bulk H/He envelope fraction.” They offer a method to estimate
the likely composition of low-mass transiting planets simply on the basis of
radius. This is an extremely useful contribution, because for the vast majority
of Kepler candidates, radius and orbital period are the only reliable
information we have.
LF13 find that the
maximum size for a typical rocky planet is 1.75 Earth radii (Rea). Although
some planets more massive than 5 Earth masses (Mea) may have radii larger than
2 Rea because they consist primarily of ices, with no appreciable contribution
from H/He, the vast majority of planets with a substantial rocky component must
be smaller than 1.75 Rea. It follows that most planets larger than 2 Rea must
have some percentage of H/He in their atmospheres. A well-known example is Kepler-22b,
announced in 2011 and sometimes described as a “habitable Super Earth.” According
to LF13, however, this object would be a miniature version of Uranus, given its
radius of 2.2 Rea.
LF13 describe
a hypothetical planet with a radius of 2 Rea and an orbit within its system’s classical
habitable zone. Assuming a rocky core and an overall mass of 5 Mea, 0.5% of the
planet’s total mass must be H/He. This tiny fraction creates an atmospheric
pressure of about 20 kilobars of H/He, which as LF13 say is 20 times higher
than the pressure at the bottom of the Marianas Trench, the deepest fissure in Earth’s
global ocean. In the habitable zone, such an atmosphere will produce surface
temperatures around 3000 K, more than 10 times higher than the mean surface
temperature on Earth (288 K). This environment is hostile to liquid water and carbon-based
life.
Figure 1. Puffy Planets. Selected transiting
planets between 3 and 7 Earth radii, with estimated fractions of
hydrogen/helium (H/He). All values except for Neptune are taken from Lopez &
Fortney 2013. The approximate H/He fraction for Neptune is inferred from their
Table 3.
The
astronomer Robin Wordsworth has presented a sceario in which a rocky planet of
5 Mea with a dissipating hydrogen atmosphere, orbiting a Sun-like star at a
distance of 2.5 AU (i.e., well outside the classical habitable zone, near the
system ice line), will experience a transient but potentially significant epoch
during which it might sustain liquid water. However, this optimistic model
seems to suffer from fine-tuning. As even Wordsworth concludes, when it comes
to hydrogen, “usually, either far too much or too little of it is present”
(Wordsworth 2012). For Kepler planets larger than 2 Rea, it’s “far too much.”
degeneracy on ice
A few
years ago, virtually everyone assumed that some subset – maybe the majority –
of Super Earths would be “Water
Planets” or “Ocean
Planets.” The consensus has changed dramatically since the discovery of the
Kepler-11
system in 2011. Now investigators routinely model rocky planets with H/He
envelopes, while the likelihood of Water Planets is questioned. Nevertheless,
LF13 accept the possibility of rock/ice planets, noting that a planet of 10 Mea
consisting of 20% rock/metal and 80% water would have a radius of 2.7 Rea. They
concede that their model suffers from the same “degeneracy” as previous efforts
when it comes to distinguishing icy planets from gassy planets. In other words,
the same radius could correspond to very different compositions.
For
example, 55 Cancri e has a measured mass and radius of 8.3 Mea and 1.99 Rea,
respectively, and is sometimes proposed as a Water Planet (Dragomir et al.
2013). Since its temperature is about 2000 K and its age is around twice that
of the Solar System, Diana Dragomir and colleagues argue that a trace hydrogen
envelope would have dissipated eons ago, while a substantial fraction of ices
might remain.
Without
providing a rationale, LF13 model 55 Cancri e as a rocky object instead, proposing
a modest H/He envelope amounting to only 0.14% of its bulk composition. However,
they leave open the possibility that other planets between 2 and 3 Rea might
qualify as Water Planets (and thus Super Earths), as long as they have a large enough
fraction of ices in their composition.
If
they exist, planets that contain a significant fraction of water or
high-pressure ices, but lack a H/He envelope, are of great scientific interest.
Nevertheless, they appear to have little relevance for astrobiology. A growing
consensus holds that, in order to maintain bodies of liquid water, a rocky
planet requires both plate tectonics and a carbon cycle. Neither is possible on
the Water Planets proposed by contemporary theorists. An object of 5 Mea whose
bulk composition is 25% water will have a differentiated structure, with a
rock/metal core surrounded by a layer of high-pressure ice thousands of
kilometers thick. This layer would block chemical interactions between
atmospheric gases and heavy elements in deeper strata, preventing the
development of a carbon cycle (Lammer et al. 2010, Alibert 2013). Yann Alibert
finds that a planet of Earth mass and composition can maintain both a global
ocean and a carbon cycle only if its water content is 2% or less, with the
maximum percentage decreasing with increasing mass (Alibert 2013).
In
addition, many astrobiologists assume that plate tectonics requires liquid
water rather than ice to lubricate continental plates (Korenaga 2010, Lammer et
al. 2010). Also widely endorsed is the argument that solid objects above a few
times the mass of the Earth, even if they somehow retained thin envelopes of
water, cannot support plate tectonics at all (O’Neill & Lenardic 2007, Morard
et al. 2011, Stein et al. 2013). Ocean Planets look less and less attractive than they
used to.
low-mass cousins
To
illustrate their model, LF13 present a table summarizing all confirmed exoplanets smaller
than Saturn with reliably measured masses and radii. Although this
sample is too small to yield robust statistics, suggestive trends are evident.
The six planets with radii between 1 and 2 Rea (where LF13 place the transition
from Super Earths to Neptune-like planets) range in mass from 1.9 to 8.45 Mea,
with a mean of 5.8 Mea and a median of 6 Mea. The corresponding mass values are
remarkably similar for the six planets between 2 and 3 Rea, which LF13 call
“sub-Neptunes” and which others have shown to represent the most numerous population
of Kepler planets (Petigura et al. 2013). For these planets, the range in mass is
2 to 7.86 Mea, the mean is 5.6 Mea, and the median is 6.7 Mea. According to LF13, objects in this group have mass fractions of H/He ranging from 0.31% to 5%, substantially
smaller than the fractions for Uranus and Neptune.
For the
12 planets between 3 and 7 Rea, which by all agreement have H/He envelopes, masses
range widely, rising from 7.3 Mea to 68.6 Mea, with a mean of 20.6 Mea and a median
of 16.8 Mea. However, confirmed exoplanets are sparse between 25 and 60 Mea; LF13 offer only three examples, none of them between 27 and 40 Mea. Such a
gap in the distribution justifies removal of the most obvious outlier, CoRoT-8b.
With a mass of almost 70 Mea, CoRoT-8b resembles a gas giant, but its unexpectedly
small radius of 6.38 Rea implies a composition dominated by heavy elements.
LH13 list its bulk composition as only one-third H/He. If we eliminate CoRoT-8b
from the sample of Neptune-like objects, the mass range becomes 7.3 to 26.2 Mea
and the mean becomes 14.9 Mea, while the median remains almost the same at 16.3
Mea. A representative sample of this group is illustrated above in Figure 1.
inner system regulars
The
latest Kepler data show that puffy planets of 3 to 7 Rea are common within 1
astronomical unit (AU) of Sun-like stars. Objects in this range of radii, as we
just saw, have a median mass very similar to Neptune’s. A number of recent
studies have calculated the distribution of these planets and their smaller,
lower-mass siblings.
Andrew
Youdin found that 3 Rea marks a clear divide in the distribution of low-mass
planets on short-period orbits (< 50 days) around Sun-like stars (Youdin
2011). Planets of this approximate radius are extremely rare on periods shorter
than 7 days, whereas both smaller and larger planets are plentiful in the same orbital
space. Youdin interpreted this distribution as a probable result of the thermal
evolution of H/He envelopes around low-mass planets that migrate to the
immediate vicinity of their host stars. Planets of the lowest mass (less than
about 8 Mea) will lose their envelopes completely, leaving bare rocky spheres
smaller than 2 Rea. More massive planets with more substantial cores can
sustain lightweight atmospheres against stripping, resulting in final radii
larger than 3 Rea.
In a more
recent analysis using a larger set of Kepler data, Subo Dong and Zhaohuan Zhu characterize
the planet population within 0.75 AU of Sun-like stars. This boundary corresponds
to an orbit of about 250 days, similar to the orbit of Venus (225 days). They
find that planets smaller than 4 Rea have a relatively flat distribution at
periods longer than 10 days, whereas planets of 4-8 Rea have a steadily
increasing distribution at longer periods (Dong & Zhu 2013). In general,
they observe, the relative fraction of “big planets” (those of 3 Rea or more)
increases with increasing period, but the increase is most pronounced for planets
smaller than 10 Rea (i.e., Saturn-size or less).
Dong
and Zhu provide an illuminating overview of the cumulative frequencies of
planets of all sizes in the Kepler sample. Within 0.75 AU, planets of 1-2 Rea (which they call
“Earth-size”) have a frequency of 28%; those of 2-4 Rea (“super-Earth-size”) have a very similar frequency, at 25%; those of 4-8 Rea (“Neptune-size”)
are far less common, at 7%; while those larger than 8 Rea
(“Jupiter-size”) are the least common of all, at only 3%.
The
relative abundance of dwarfs and rarity of giants has been widely observed. It
is rapidly becoming a cornerstone of exoplanetary science, analogous to the abundance
of lower-mass stars (M dwarfs) versus their higher-mass (O and B-type)
siblings.
REFERENCES
Alibert Y. (2013) On the radius of habitable planets. Astronomy & Astrophysics, in press.
Dragomir D, Matthews JM, Winn JN, Rowe JF, MOST Science Team
(2013) New MOST photometry of the 55 Cancri system. In press. Abstract: http://adsabs.harvard.edu/abs/2013arXiv1302.3321D
Dong S &
Zhu Z. (2013) Fast rise of
“Neptune-size” planets (4-8 Rearth) from P ∼10
to ∼250
days: Statistics of Kepler planet candidates up to ∼0.75 AU. Astrophysical Journal 778, 53.
Korenaga
J. (2010) On the
likelihood of plate tectonics on Super-Earths: Does size matter? Astrophysical Journal Letters 725, L43-L46.
Lammer H, Selsis F, Chassefiere E, Breuer D, Griessmeier J-M,
Kulikov YN, et al. (2010) Geophysical and atmospheric evolution of habitable
planets. Astrobiology 10, 45-68.
Lopez ED
& Fortney JJ. (2013) Understanding
the mass-radius relation for sub-Neptunes: Radius as a proxy for composition. In
press. Abstract: http://adsabs.harvard.edu/abs/2013arXiv1311.0329L
O’Neill C
& Lenardic A. (2007) Geological
consequences of super-sized Earths. Geophysical
Research Letters 34.
Morard
G, Bouchet
F, Valencia D,
Mazevet S, Guyot F. (2011) The melting curve of
iron at extreme pressures: Implications for planetary cores. High Energy
Density Physics 7, 141-144.
Petigura EA, Geoffrey MW, Howard AW. (2013) A plateau in the
planet population below twice the size of Earth. Astrophysical Journal 770, 69. Abstract: http://adsabs.harvard.edu/abs/2013ApJ...770...69P
Stein C, Lowman JP, Hansen U. (2013). The influence of mantle
internal heating on lithospheric mobility: Implications for super-Earths. Earth and Planetary Science Letters 361,
448-459.
Wordsworth
R. (2012) Transient conditions for
biogenesis on low-mass exoplanets with escaping hydrogen atmospheres. Icarus 219, 267-273.
Youdin AN.
(2013) The exoplanet census: A general method applied to Kepler. Astrophysical Journal 742, 38. Abstract: http://adsabs.harvard.edu/abs/2011ApJ...742...38Y
No comments:
Post a Comment