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Starts With A Bang

What’s Left Behind When You Boil A Gas Giant?

When large, massive, gas giant exoplanets come too close to their parent star, the outer gas envelope can be mostly or entirely stripped away. What remains might be an exposed planetary core, not much bigger than Earth but comparable in mass to a world like Neptune or Uranus. (MARK GARLICK / UNIVERSITY OF WARWICK)

There are exposed planetary cores orbiting stars, and we may have already found them.


When we take a look at the planets in our Solar System, there’s a pretty clear difference between the four inner, rocky worlds and the outer, gaseous, giant planets. Mercury, Venus, Earth and Mars are all small, low in mass, and dense, with atmospheres that represent only a tiny fraction-of-a-percent of the planet’s overall matter. On the other hand, Jupiter, Saturn, Uranus and Neptune are comparatively giant, heavy, but diffuse, with the majority of their mass contained in an enormous, gas-rich envelope made mostly of hydrogen and helium.

But deep inside the giant worlds of our Solar System, beneath the various layers of volatile gases, lies a massive core rich in heavy elements. Each one contains a rocky core that’s significantly more massive than any of the “rocky” planets in our Solar System, with the gravitational force sufficient — at their great distances from the Sun — to hold onto the light elements in their outer atmospheres. But not every gas giant is so lucky; some of them should be too close to their parent stars, where their volatile gas atmospheres are boiled away. Here’s what’s left behind.

Protoplanetary disks, which all solar systems are thought to form with, will coalesce into planets over time, as this illustration shows. It’s important to recognize that the central star, the individual planets, and the leftover primordial material (which will, for example, become asteroids or Kuiper belt objects) may all have variations in ages on the order of tens of millions of years. (NAOJ)

If we want to understand how our Solar System came to be — or any solar system in the Universe — we have to rewind the clock all the way back to when they first form. We start with a cloud of cool gas that begins to collapse under its own gravity, which is what’s needed to trigger the formation of new stars. Any one system will result from the fragmentation of a cloud into a small chunk, which will preferentially collapse along the shortest dimension first. As long as the enough of the gas can cool sufficiently, you’ll wind up with one or more stars forming near the central location.

But in the more outer regions, a number of different effects all compete for dominance. The outer material also collapses along its shortest direction, leading to the formation of a protoplanetary disk. Collisions between various particles pull the heavier, denser ones closer to the center, while leaving the lighter, less dense ones more evenly distributed. Heat from the central proto-star radiates outward, blowing off the lightest, least dense material closest to the proto-star itself. And gravitational instabilities attempt to grow, while random collisions blast proto-planets apart and gravitational interactions eject a significant fraction of them.

In the cosmic race to form planets from this material before the central star(s) become too hot and luminous, blowing the planet-forming material out of the solar system entirely, there are winners and losers. From a planetary perspective, the “winners” meet the International Astronomical Union’s definition of a planet, as extended to exoplanetary systems. This includes:

  1. it orbits its central star and no other bodies,
  2. it’s massive enough to achieve hydrostatic equilibrium: pulling itself into a spheroidal shape defined by its gravity, composition, and rotation,
  3. and it clears its own orbit on timescales comparable to the age of the star system in question.
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While the original 2006 definition unceremoniously resulted in the “demotion” of then-planet Pluto, causing some controversy, subsequent work by planetary astronomers and exoplanet scientists have validated the usefulness of this definition. If you’re large enough, massive enough, dominant enough, and in the right location in your solar system, congratulations: you’re a planet.

If you want to be classified as a planet, you need to have a certain combination of mass and orbital distance relative to your parent star. In 2015, Jean-Luc Margot extended the IAU’s definition to include exoplanets in a clean and compelling single relationship that is still valid today. (MARGOT (2015), VIA HTTP://ARXIV.ORG/ABS/1507.06300)

When it comes to how to classify these worlds, however, scientists didn’t find what they were expecting. In the early stages of exoplanet astronomy, many suspected that the planets we’d find around other stars would be similar to the ones in the Solar System. Very quickly, however, that idea was turned on its head, as the first planets that came back were:

  • very massive, more massive than even Jupiter,
  • very close to their parent star, orbiting faster and at smaller distances than Mercury,
  • and extraordinarily hot, with surface temperatures rising into the thousands of degrees: hotter than any world in our Solar System by far.

These so-called “hot Jupiters” were the first types of surprising exoplanets discovered, but were far from the last. The most common planet type found was actually in between the sizes of Earth and Uranus, causing astronomers to invent a new category: either “super-Earth” or “mini-Neptune,” depending on who you ask.

Although more than 4,000 confirmed exoplanets are known, with more than half of them uncovered by Kepler, finding a Mercury-like world around a star like our Sun is well beyond the capabilities of our current planet-finding technology. As viewed by Kepler, Mercury would appear to be 1/285th the size of the Sun, making it even more difficult than the 1/194th size we see from Earth’s point of view. (NASA/AMES RESEARCH CENTER/JESSIE DOTSON AND WENDY STENZEL; MISSING EARTH-LIKE WORLDS BY E. SIEGEL)

These initial categories, unfortunately, were biased by our own expectations, and didn’t necessarily represent anything that was physically real other than our preconceived prejudices. Since we began detecting exoplanets directly some 30 years ago, we’ve catalogued more than 4,000 of them, learning unprecedented information about their masses, radii, and where in orbit around their parent star they form.

What we found is that large bodies of any mass/size combination can form at any distance from their star, but that when you look at the mass/size combinations themselves, they point to four general categories:

  1. terrestrial/rocky planets, without large gas envelopes, with masses up to about twice that of Earth,
  2. smaller gas-dominated planets, like Uranus, Neptune, or even Saturn, with masses ranging from two Earth masses up to about 130 Earth masses,
  3. gas giant planets that exhibit gravitational self-compression, like Jupiter, with masses from ~40% that of Jupiter up to ~8% the mass of our Sun,
  4. and full-blown stars, of 8% the Sun’s mass or greater, where nuclear fusion has ignited in the core.
The classification scheme of planets as either rocky, Neptune-like, Jupiter-like or stellar-like. Although we created a large number of artificial categories initially, such as sub-terran or super-Earth worlds, the data supports that there are only three main class of planet: terran worlds, neptunian worlds, and jovian worlds. (CHEN AND KIPPING, 2016)

Although the science of how these planets form remains in the early stages, we at least have a working hypothesis. From the initial gravitational instabilities in a protoplanetary disk, the following steps can occur:

  • a gravitational instability becomes dense enough that it starts to attract the matter in or near its orbit,
  • where it begins to grow into a rocky core, similar in material to Earth’s mantle, with denser material sinking to the protoplanet’s center,
  • with the core attempting to grow against the competing forces of evaporative solar radiation and the attempts of large, neighboring instabilities to collect that material instead.

There appears to be a threshold: once the mass of your core gets to about 10 Earth masses or more, it will start to accrue large amounts of hydrogen and helium very quickly, leading to the possibility of it growing into a gas giant with self-compression. Below that threshold, and you might still make it to a hydrogen/helium envelope, but you’re more likely to be Neptune-sized than Jupiter-sized.

A cutaway of Jupiter’s interior. If all the atmospheric layers were stripped away, the core would appear to be a rocky super-Earth, but with an extremely high density. Planets that formed with fewer heavy elements can be a lot larger and less dense than Jupiter. (WIKIMEDIA COMMONS USER KELVINSONG)

In our own Solar System, the cores of Neptune and Uranus failed to meet this threshold, while Jupiter likely passed it quite early. Saturn is a sort of in-between case, as its core has an uncertain mass that may fall either below or above that threshold, but is close in either case.

But in other solar systems, there are a few outliers that don’t follow these trends exactly. In particular, there are quite a few exoplanets known that are between 1 and 2 Earth radii, but can be many times the mass of Earth: up to 20 Earth masses or so!

That’s like having a planet equal to the mass of Neptune or Uranus, but contained in a volume that’s only a few times larger than Earth’s. In other words, these planets have to have densities comparable to or even greater than our own planet’s, meaning they must be composed almost entire of rocky/metallic material.

A visualization of the exoplanet Kepler-107c by NASA almost certainly doesn’t have clouds or stripes on it, as it’s most likely an ultra-hot planet that’s far denser and more massive than Earth, despite being only marginally larger in size. It is one of the densest exoplanets ever discovered, likely resulting from a stripped gas giant’s core. (NASA / EXOPLANET EXPLORATION PROGRAM / JPL)

Planets such as this, interestingly enough, are almost exclusively found very close to their parent star. One such example is Kepler-107c, which comes in at 9.4 times the mass of Earth, but is just 60% larger in radius than our planet. This means its density is a whopping 2.3 times the density of Earth: denser, on average, than silver, lead, or even mercury. (Not Mercury the planet; mercury the periodic table element.)

The only reasonable way for this to form is if this exoplanet is the stripped core of a gas giant: one that has been too close to its parent star for too long to hang onto its hydrogen and helium envelope. Considering that this planet orbits a Sun-like star of similar mass and temperature to our own, but completes a full orbit in just 4.9 days, this is a relatively likely scenario. Many other such examples are known to exist, and studying planets like this can teach us what a “stripped core” of a gas giant might actually look like.

Small but very massive planets, such as TOI 849b, have been discovered, indicating that they are likely stripped cores of gas giant worlds based on their densities and proximities to their parent stars. These worlds might represent an uncommon fourth class of planet, but further observations are necessary to know for certain. (NASA / JPL-CALTECH)

One of the most exciting prospects for a stripped-core world like this will come with the advent of 30-meter class telescopes on the ground: direct imaging of worlds just a little bit larger than Earth. That could include — even for small planet-star separation distances (if the star is close enough) — planets such as:

  • gas giants, both with and without self-compression,
  • stripped-core planets that were once gas giants,
  • and possibly even the largest of the rocky, terrestrial-like planets.

While we might need yet another leap forward in telescope technology, such as the space-based HabEx or LUVOIR proposals, to image an Earth-sized world around a Sun-like star directly, it’s definitely within the realm of possibility for the 2030s. If we choose to invest in it, we can learn not only about the Earth-like worlds in our vicinity, but the most spectacular planetary outliers as well.

If the Sun were located 10 parsecs (33 light years) away, not only would LUVOIR be able to directly image Jupiter and Earth, including taking their spectra, but even the planet Venus would yield to observations. A significantly closer Sun-like star could even reveal a potential stripped-core world if the orbital parameters were favorable. (NASA / LUVOIR CONCEPT TEAM)

For generations, we assumed that if there were planets around stars other than the Sun, they might follow the same generic pattern that we observe here: inner, rocky planets, outer, gas giant planets, with asteroids in between and icy worlds beyond them all. With the first few thousand planets under our belt, we now know that our Solar System isn’t typical at all, and that planets come in a wide variety of masses, radii, and orbital distances. Moreover, they fall into not two, but three general categories: rocky worlds, small gas giants with hydrogen/helium envelopes, and massive gas giants that exhibit self-compression.

But there are also outliers: cases where a planet experiences extreme conditions that creates an outcome that doesn’t land squarely in one of these three categories. In addition to planets on or near the borders between different categories, such as Saturn, there are planets whose growth is stunted or whose evolution is irrevocably altered by collisions, gravitational encounters, or an incredibly close proximity to their parent star. After decades of research, we’re finally close to understanding how planets in the Universe come to be. Soon, with upcoming technology, we’ll finally learn what these boiled-off gas giants are truly like.


Ethan Siegel is the author of Beyond the Galaxy and Treknology. You can pre-order his third book, currently in development: the Encyclopaedia Cosmologica.

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