
Star formation is the process by which dense regions within molecular clouds collapse to form new stars.Star formation is a multi-stage process triggered in the densest cores of giant molecular clouds (with masses up to 10⁶ solar masses). External influences — spiral density waves, shock waves from supernovae, cloud collisions — create local over-densities. Gravitational instability overcomes the combined support of thermal pressure, magnetic fields, and turbulence. The initial isothermal collapse transitions to adiabatic when the core becomes opaque to its own radiation. A protostar forms with an accretion disk and bipolar outflows. When the central temperature reaches millions of degrees, deuterium ignites first, and at ~10⁷ K, hydrogen ignites in the pp-chain or CNO cycle. The star arrives on the main sequence, where it spends almost its entire life. The mass distribution of newborns (the initial mass function) is roughly universal: many low-mass and very few massive stars.
The nebular hypothesis was proposed in the 18th century by Swedenborg, Kant, and Laplace. In the early 20th century, James Jeans examined the gravitational instability of a homogeneous medium (Jeans criterion). The discovery of dark nebulae by Barnard and others confirmed the existence of cold clouds. Infrared astronomy (IRAS, Spitzer, Herschel) in the 1970s–2010s revealed protostars, and the ALMA interferometer allowed seeing disks and jets in detail. Subrahmanyan Chandrasekhar made a fundamental contribution to the theory of stellar structure and evolution, formulating the Chandrasekhar limit for white dwarfs.
Star formation is governed by the balance of gravity, pressure, magnetic fields, and turbulence. Jeans criterion: a cloud of mass M collapses if M > M_J = (π/6) c_s³ G^(-3/2) ρ^(-1/2). In magnetized media, the critical mass-to-magnetic flux ratio must be exceeded. Efficient cooling via dust emission in the far-IR ensures isothermality of the early collapse. Once the optical depth reaches about unity, the core heats up. Conservation of angular momentum leads to the formation of an accretion disk; magnetic braking can reduce it. Accretion onto the protostar generates shock waves emitting in the UV and optical. At ~10⁶ K, deuterium ignites; at ~10⁷ K, hydrogen ignites. For massive stars, radiation pressure plays a role, which can halt spherical accretion; material falls through the disk. Bipolar outflows (jets) carry away excess material and angular momentum. On galactic scales, the star formation rate is related to the gas surface density by the empirical Kennicutt-Schmidt law: Σ_SFR ∝ Σ_gas^n, where n ≈ 1.4. Key equations: hydrostatic equilibrium dP/dr = -G M_r ρ/r², continuity equation, energy transport and nuclear energy generation equations, equation of state (ideal gas with radiation pressure), opacity. The initial mass function (IMF) results from turbulent fragmentation and thermal physics; the IMF Salpeter law is often used for high masses.
Understanding the mechanisms of star formation is necessary to explain why galaxies look the way they do, where the chemical elements that make up us and our planet come from, and to predict the prevalence of planetary systems.
The Orion Nebula is the nearest 'stellar nursery' to us (about 1300 light-years away), where among the glowing gas one can see protoplanetary disks like dark silhouettes against a bright background. Planets are assembling in them right now.





















