Stars form from interstellar gas clouds, with accretion flows feeding their growth.Star formation begins in cold, dense regions of interstellar gas clouds, primarily composed of molecular hydrogen and dust. These clouds collapse under their own gravity, fragmenting into cores that eventually ignite nuclear fusion. The process is not uniform: accretion flows channel gas onto the forming protostar, while feedback from stellar winds and radiation can both trigger and quench further star formation. This cycle of gas collapse and feedback shapes galaxies, determining their structure and evolution over cosmic time.
The modern theory of star formation from gas clouds was developed in the mid-20th century, with key contributions from Lyman Spitzer and others who studied the interstellar medium. The role of accretion disks was clarified in the 1970s and 1980s through observations and theoretical models.
A molecular cloud becomes gravitationally unstable when its internal pressure can no longer counteract gravity, often triggered by shock waves from supernovae or galaxy collisions. As the cloud collapses, it fragments into dense cores, each of which accretes material from a surrounding disk. The infalling gas releases gravitational energy, heating the core until temperatures reach millions of degrees, igniting hydrogen fusion. The newly formed star then emits radiation and winds that disperse the remaining gas, halting further accretion and potentially triggering star formation in neighboring regions.
Understanding star formation is essential for modeling galaxy evolution, interpreting observations of distant galaxies, and identifying potentially habitable planetary systems around young stars.
The most massive stars form so quickly that they can exhaust their fuel and explode as supernovae in less than a few million years, while the smallest red dwarfs can burn for trillions of years.
| f'_λ | variable | observed flux at wavelength λ after extinction — flux watt per square metre |
| f_λ | variable | intrinsic flux at wavelength λ before extinction — flux watt per square metre |
| A_λ | variable | extinction magnitude at wavelength λ — extinction magnitude |






















