Formation, orbital and thermal evolution, and survival of planetary-mass clumps in the early phase of circumstellar disk evolution
We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the formation and evolution of the circumstellar disk and the clumps formed by disk fragmentation. Our simulation shows that disk fragmentation occurs in...
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Abstract | We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the formation and evolution of the circumstellar disk and the clumps formed by disk fragmentation. Our simulation shows that disk fragmentation occurs in the early phase of circumstellar disk evolution and many clumps form. The clump can be represented by a polytrope sphere of index \(n \sim 3\) and \(n \gtrsim 4\) at central temperature \(T_c \lesssim100\) K and \(T_c \gtrsim 100\) K, respectively. We demonstrate, numerically and theoretically, that the maximum mass of the clump, beyond which it inevitably collapses, is \(\sim 0.03 M_{\odot}\). The entropy of the clump increases during its evolution, implying that evolution is chiefly determined by mass accretion from the disk rather than by radiative cooling. Although most of the clumps rapidly migrate inward and finally fall onto the protostar, a few clumps remain in the disk. The central density and temperature of the surviving clump rapidly increase and the clump undergoes a second collapse within 1000 - 2000 years after its formation. In our simulation, three second cores of masses \(0.2\msun\), \(0.15\msun\), and \(0.06\msun\) formed. These are protostars or brown dwarfs rather than protoplanets. For the clumps to survive as planetary-mass objects, the rapid mass accretion should be prevented by some mechanisms. |
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AbstractList | We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the formation and evolution of the circumstellar disk and the clumps formed by disk fragmentation. Our simulation shows that disk fragmentation occurs in the early phase of circumstellar disk evolution and many clumps form. The clump can be represented by a polytrope sphere of index \(n \sim 3\) and \(n \gtrsim 4\) at central temperature \(T_c \lesssim100\) K and \(T_c \gtrsim 100\) K, respectively. We demonstrate, numerically and theoretically, that the maximum mass of the clump, beyond which it inevitably collapses, is \(\sim 0.03 M_{\odot}\). The entropy of the clump increases during its evolution, implying that evolution is chiefly determined by mass accretion from the disk rather than by radiative cooling. Although most of the clumps rapidly migrate inward and finally fall onto the protostar, a few clumps remain in the disk. The central density and temperature of the surviving clump rapidly increase and the clump undergoes a second collapse within 1000 - 2000 years after its formation. In our simulation, three second cores of masses \(0.2\msun\), \(0.15\msun\), and \(0.06\msun\) formed. These are protostars or brown dwarfs rather than protoplanets. For the clumps to survive as planetary-mass objects, the rapid mass accretion should be prevented by some mechanisms. We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the formation and evolution of the circumstellar disk and the clumps formed by disk fragmentation. Our simulation shows that disk fragmentation occurs in the early phase of circumstellar disk evolution and many clumps form. The clump can be represented by a polytrope sphere of index $n \sim 3$ and $n \gtrsim 4$ at central temperature $T_c \lesssim100$ K and $T_c \gtrsim 100$ K, respectively. We demonstrate, numerically and theoretically, that the maximum mass of the clump, beyond which it inevitably collapses, is $\sim 0.03 M_{\odot}$. The entropy of the clump increases during its evolution, implying that evolution is chiefly determined by mass accretion from the disk rather than by radiative cooling. Although most of the clumps rapidly migrate inward and finally fall onto the protostar, a few clumps remain in the disk. The central density and temperature of the surviving clump rapidly increase and the clump undergoes a second collapse within 1000 - 2000 years after its formation. In our simulation, three second cores of masses $0.2\msun$, $0.15\msun$, and $0.06\msun$ formed. These are protostars or brown dwarfs rather than protoplanets. For the clumps to survive as planetary-mass objects, the rapid mass accretion should be prevented by some mechanisms. |
Author | Tsukamoto, Yusuke Inutsuka, Shuichiro Machida, Masahiro N |
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BackLink | https://doi.org/10.48550/arXiv.1307.6910$$DView paper in arXiv https://doi.org/10.1093/mnras/stt1684$$DView published paper (Access to full text may be restricted) |
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Snippet | We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the... We report the results of our three-dimensional radiation hydrodynamics simulation of collapsing unmagnetized molecular cloud cores. We investigate the... |
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SubjectTerms | Accretion disks Brown dwarf stars Clumps Computational fluid dynamics Computer simulation Fluid flow Fragmentation Hydrodynamics Molecular clouds Physics - Earth and Planetary Astrophysics Physics - Solar and Stellar Astrophysics Planet formation Planetary evolution Protoplanets Protostars Simulation Star formation Survival Thermal evolution |
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Title | Formation, orbital and thermal evolution, and survival of planetary-mass clumps in the early phase of circumstellar disk evolution |
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