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Gravitational collapse
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==Star formation== {{Main|Star formation}} An interstellar cloud of gas will remain in [[hydrostatic equilibrium]] as long as the [[kinetic energy]] of the gas [[pressure]] is in balance with the [[potential energy]] of the internal [[gravitational force]]. Mathematically this is expressed using the [[virial theorem]], which states that to maintain equilibrium, the gravitational potential energy must equal twice the internal thermal energy.<ref>{{cite book | first=Sun | last=Kwok | date=2006 | title=Physics and chemistry of the interstellar medium | url=https://archive.org/details/physicschemistry0000kwok | url-access=registration | publisher=University Science Books | isbn=1-891389-46-7 | pages=[https://archive.org/details/physicschemistry0000kwok/page/435 435β437] }}</ref> If a pocket of gas is massive enough that the gas pressure is insufficient to support it, the cloud will undergo gravitational collapse. The critical mass above which a cloud will undergo such collapse is called the [[Jeans mass]]. This mass depends on the temperature and density of the cloud but is typically thousands to tens of thousands of [[solar mass]]es.<ref>{{cite book | first=Dina | last=Prialnik | title=An Introduction to the Theory of Stellar Structure and Evolution | publisher=[[Cambridge University Press]] | date=2000 | isbn=0-521-65937-X | pages=198β199 }}</ref>
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