Gas Giant Planet

Author(s):  
Daniel Rouan
Keyword(s):  
2011 ◽  
Vol 740 (2) ◽  
pp. 76 ◽  
Author(s):  
I. Ramírez ◽  
J. Meléndez ◽  
D. Cornejo ◽  
I. U. Roederer ◽  
J. R. Fish

Author(s):  
Morris Podolak

Modern observational techniques are still not powerful enough to directly view planet formation, and so it is necessary to rely on theory. However, observations do give two important clues to the formation process. The first is that the most primitive form of material in interstellar space exists as a dilute gas. Some of this gas is unstable against gravitational collapse, and begins to contract. Because the angular momentum of the gas is not zero, it contracts along the spin axis, but remains extended in the plane perpendicular to that axis, so that a disk is formed. Viscous processes in the disk carry most of the mass into the center where a star eventually forms. In the process, almost as a by-product, a planetary system is formed as well. The second clue is the time required. Young stars are indeed observed to have gas disks, composed mostly of hydrogen and helium, surrounding them, and observations tell us that these disks dissipate after about 5 to 10 million years. If planets like Jupiter and Saturn, which are very rich in hydrogen and helium, are to form in such a disk, they must accrete their gas within 5 million years of the time of the formation of the disk. Any formation scenario one proposes must produce Jupiter in that time, although the terrestrial planets, which don’t contain significant amounts of hydrogen and helium, could have taken longer to build. Modern estimates for the formation time of the Earth are of the order of 100 million years. To date there are two main candidate theories for producing Jupiter-like planets. The core accretion (CA) scenario supposes that any solid materials in the disk slowly coagulate into protoplanetary cores with progressively larger masses. If the core remains small enough it won’t have a strong enough gravitational force to attract gas from the surrounding disk, and the result will be a terrestrial planet. If the core grows large enough (of the order of ten Earth masses), and the disk has not yet dissipated, then the planetary embryo can attract gas from the surrounding disk and grow to be a gas giant. If the disk dissipates before the process is complete, the result will be an object like Uranus or Neptune, which has a small, but significant, complement of hydrogen and helium. The main question is whether the protoplanetary core can grow large enough before the disk dissipates. A second scenario is the disk instability (DI) scenario. This scenario posits that the disk itself is unstable and tends to develop regions of higher than normal density. Such regions collapse under their own gravity to form Jupiter-mass protoplanets. In the DI scenario a Jupiter-mass clump of gas can form—in several hundred years which will eventually contract into a gas giant planet. The difficulty here is to bring the disk to a condition where such instabilities will form. Now that we have discovered nearly 3000 planetary systems, there will be numerous examples against which to test these scenarios.


2017 ◽  
Vol 13 (S332) ◽  
pp. 109-112
Author(s):  
Rafael Pinotti ◽  
Heloisa M. Boechat-Roberty ◽  
Gustavo F. Porto de Mello

AbstractIn 2005 we suggested a relation between the optimal locus of gas giant planet formation, prior to migration, and the metallicity of the host star, based on the core accretion model, and radial profiles of dust surface density and gas temperature. At that time, less than 200 extrasolar planets were known, limiting the scope of our analysis. Here, we take into account the expanded statistics allowed by new discoveries, in order to check the validity of some premises. We compare predictions with the present available data and results for different stellar mass ranges. We find that the zero age planetary orbit (ZAPO) hypothesis continues to hold after a two order of magnitude increase in discovered planets, as well as the prediction that planets around metal poor stars would have shorter orbits.


2019 ◽  
Vol 491 (3) ◽  
pp. 4481-4487
Author(s):  
Ares Osborn ◽  
Daniel Bayliss

ABSTRACT We investigate the giant planet–metallicity correlation for a homogeneous, unbiased set of 217 hot Jupiters taken from nearly 15 yr of wide-field ground-based surveys. We compare the host star metallicity to that of field stars using the Besançon Galaxy model, allowing for a metallicity measurement offset between the two sets. We find that hot Jupiters preferentially orbit metal-rich stars. However, we find the correlation consistent, though marginally weaker, for hot Jupiters ($\beta =0.71^{+0.56}_{-0.34}$) than it is for other longer period gas giant planets from radial velocity surveys. This suggests that the population of hot Jupiters probably formed in a similar process to other gas giant planets, and differ only in their migration histories.


2009 ◽  
Vol 698 (1) ◽  
pp. 1-27 ◽  
Author(s):  
Thayne Currie ◽  
Charles J. Lada ◽  
Peter Plavchan ◽  
Thomas P. Robitaille ◽  
Jonathan Irwin ◽  
...  

Author(s):  
Masahiro N. Machida ◽  
Eiichiro Kokubo ◽  
Shu-ichiro Inutsuka ◽  
Tomoaki Matsumoto
Keyword(s):  

Icarus ◽  
2005 ◽  
Vol 173 (2) ◽  
pp. 417-424 ◽  
Author(s):  
R DURISEN ◽  
K CAI ◽  
A MEJIA ◽  
M PICKETT

2008 ◽  
Vol 385 (3) ◽  
pp. 1576-1584 ◽  
Author(s):  
D. Pollacco ◽  
I. Skillen ◽  
A. Collier Cameron ◽  
B. Loeillet ◽  
H. C. Stempels ◽  
...  
Keyword(s):  

2018 ◽  
Vol 363 (9) ◽  
Author(s):  
Chunjian Liu ◽  
Qing Ai ◽  
Zhen Yao ◽  
Hualian Tian ◽  
Jiayun Shen ◽  
...  

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