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The 1944 accretion model by Otto Schmidt was further developed in a quantitative way in 1969 by Viktor Safronov. [4] He calculated, in detail, the different stages of terrestrial planet formation. [5] [6] Since then, the model has been further developed using intensive numerical simulations to study planetesimal accumulation.
The disk eventually disappears due to accretion onto the central star, planet formation, ejection by jets and photoevaporation by UV-radiation from the central star and nearby stars. [48] As a result, the young star becomes a weakly lined T Tauri star, which slowly, over hundreds of millions of years, evolves into an ordinary Sun-like star. [38]
This process increases the cross section over which the large bodies can accrete material, accelerating their growth. The rapid growth of the planetesimals via pebble accretion allows for the formation of giant planet cores in the outer Solar System before the dispersal of the gas disk.
Gradually, gentle collisions allowed the flakes to stick together and make larger particles which, in turn, attracted more solid particles towards them. This process is known as accretion. The objects formed by accretion are called planetesimals—they act as seeds for planet formation. Initially, planetesimals were closely packed.
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The accretion process can convert about 10 percent to over 40 percent of the mass of an object into energy as compared to around 0.7 percent for nuclear fusion processes. [5] In close binary systems the more massive primary component evolves faster and has already become a white dwarf , a neutron star, or a black hole, when the less massive ...
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Core formation utilizes several mechanisms in order to control the movement of metals into the interior of a planetary body. [3] Examples include percolation, diking, diapirism, and the direct delivery of impacts are mechanisms involved in this process. [3] The metal to silicate density difference causes percolation or the movement of a metal ...