Astronomy/Exoplanets

Exoplanets, or extra-solar planets, are planets orbiting stars outside of Earth's solar system. Exoplanets is one of the two topics for the 2016 Astronomy event, the other being Star and Planet Formation.

Gas Giant
Planet composed mainly of hydrogen and helium. They may possibly have rocky or icy cores. They have masses greater than 10 Earth masses. Around 25% of all discovered exoplanets are gas giants.

Hot Jupiters
Gas giants that are orbits very close to its host star. Scientists believed Hot Jupiters formed farther away and migrated inward. Migration is a change in orbit due to interactions with a disk of gas or planetesimals. Hot Jupiters are found within .05-.5 AU of the host star. They are extremely hot, with temperatures as high as 2400 K. They are the most common type of exoplanet found because they are the easiest to detect (because they are huge and close to the host star.) Around 50% of discovered exoplanets are Hot Jupiters.

Ice Giant
Composed primarily of volatile substances heavier than helium, such as oxygen, carbon, nitrogen, and sulfur. Ice giants have significantly less helium and hydrogen than gas giants and they are also smaller. Uranus and Neptune are ice giants. According to some planetary models, these two giant planets may have a layers of superioninc ice under relatively shallow hydrogen and helium atmospheres, which would explain their unusual magnetic fields.

Terrestrial Planet
Composed primarily of silicate minerals or metals.

Super-Earth
Defined exclusively by mass with upper and lower limits. Super Earths are ‘potentially’ rocky planets with up to 10 times the mass of Earth. The term ‘Super Earth’ simply refers to the mass of the planet and not to any planetary conditions, so some of these may actually be gas dwarfs. The Kepler Mission defined a Super-Earth as a planet bigger than Earth-like planets (.8-1.25 Earth radii), but smaller than mini-Neptunes (2-4 Earth-radii).

Mini-Neptune
Also known as a gas dwarf or transitional planet. Mini-Neptunes are planets with a mass up to 10 Earth masses. They are less massive than Uranis and Neptune (shocker) and have thick hydrogen/helium atmospheres.

Pulsar Planet
A planet that orbits a pulsar, a rapidly rotating neutron star. Pulsar planets are discovered through anomalies in pulsar timing measurements. Pulsars rotate at a regular speed, so any bodies orbiting the pulsar will cause regular changes in its pulsation. The changes can be detected with precise timing measurements.

Goldilocks Planet
Planet that falls within star's habitable zone, which basically means it has liquid water.

Rogue Planet
Also known as interstellar planet, nomad planet, free-floating planet, orphan planet, wandering planet or starless planet. A planet without a host star that orbits the galaxy directly.

Puffy Planet
A planet with a large radius but very low density. Puffy planets expand because they are being warmed from the inside out. This warming may be from the star's heat reaches the planet's core, or from stellar winds carrying ions and heat that reach deeper into the planet. The ions are attracted to the planet's magnetic field. Friction is generated by winds blowing past ions being held by the magnetic field, creating heat that will warm the planet from the inside and causing it to expand.

Chthonian Planet
The rocky core left behind when a hot Jupiter orbits too close to their star. The star's heat and extreme gravity can rip away the planet's water or atmosphere.

Water Worlds
An exoplanet completely covered in water. Simulations suggest that these planets formed from ice-rich debris further from their host star. As they migrated inward, the water melted and covered the planet in a giant ocean.

Temperature of Exoplanets
In calculation of temperature of exoplanet, the star is often assumed to be a blackbody. The exoplanet is assumed to reflect some of the radiation, have no heating from its core, and have emissivity close to 1.

Let the temperature of the exoplanet and the star be [math]T_e[/math] and [math]T_s[/math], and the radius be [math]R_e[/math] and [math]R_s[/math]. They are separated by a distance of [math]D[/math]. Then, by Stefan-Boltzmann Law, the radiation from the star and the exoplanet is [math]L_s=4\pi R_s^2\cdot \sigma T_s^4, \qquad L_e=4\pi R_e^2\cdot \sigma T_e^4,[/math] where [math]\sigma[/math] is the Stefan-Boltzmann constant.

Only a fraction of the star's radiation reaches the exoplanet, and only a fraction of those radiation is absorbed. The ratio of radiation that reaches the exoplanet is [math]\frac{\pi R_e^2}{4\pi D^2}[/math] by considering the sphere centered at the sun that crosses the exoplanet, and [math]1-A[/math] of those is absorbed, where [math]A[/math] is the Albedo of the planet. Therefore, [math] L_e=\frac{\pi R_e^2(1-A)}{4\pi D^2}L_s.[/math]

Expanding [math]L_e[/math] and [math]L_s[/math] and simplifying, we find [math]T_e^4 = \frac{R_s^2T_s^4(1-A)}{4D^2}, \qquad T_e=\sqrt[4]{\frac{R_s^2T_s^4(1-A)}{4D^2}}.[/math]

For example, if both the sun and the Earth are assumed to be blackbodies ([math]A=0[/math]), the temperature of the Earth would be [math]\sqrt[4]{\frac{(7\cdot 10^8m)^2(5778K)^4}{4(1\text{AU})^2}}=280K.[/math]