
The law of conservation of angular momentum states that the total angular momentum of a closed system remains constant.Kepler already noticed in 1609 that planets sweep out equal areas in equal times — this is historically the first example of conservation of angular momentum. In 1915, Emmy Noether proved that the symmetry of space (its isotropy) leads to the conservation of this quantity. Formally: angular momentum L = Iω remains constant if the net external torque is zero.
Johannes Kepler formulated his second law (1609) — the radius vector of a planet sweeps out equal areas in equal times, which is a consequence of conservation of angular momentum. Isaac Newton in the 'Principia' derived the conservation from the laws of motion and gravity. In 1915, Emmy Noether proved a general theorem linking symmetries and conservation laws, in particular, the isotropy of space to the conservation of angular momentum.
Used everywhere: from designing gyrostabilized platforms to analyzing elementary particle collisions. Boundaries: the classical form is valid as long as quantum and relativistic corrections can be neglected. In general relativity, global conservation of angular momentum is not always well-defined due to the absence of global symmetry.
Attitude control of spacecraft (reaction wheels), sports spins, stabilization of pulsars.
A gyroscope, spun up to high speed, resists attempts to change its axis — navigation instruments operate on this principle.
| I | variable | Moment of inertia about the axis — moment of inertia kilogram metre squared |
| r | variable | Perpendicular distance from the axis to mass element — distance metre |
| dm | variable | Infinitesimal mass element — mass kilogram |
| ∫ | operator | Integration over the entire body — integral operator |
| J^{\mu\nu\alpha} | variable | Angular momentum density tensor — angular momentum density kilogram per metre per second |
| x^{\mu} | variable | Spacetime coordinate — position metre |
| x^{\nu} | variable | Spacetime coordinate — position metre |
| T^{\nu\alpha} | variable | Stress-energy tensor component — stress energy tensor joule per cubic metre |
| T^{\mu\alpha} | variable | Stress-energy tensor component — stress energy tensor joule per cubic metre |
| \dot{J} | variable | Angular momentum loss rate — angular momentum loss rate kilogram metre squared per second square |
| \dot{M} | variable | Mass transfer rate — mass transfer rate kilogram per second |
| M_1 | variable | Mass of the primary star — mass kilogram |
| M_2 | variable | Mass of the secondary star — mass kilogram |
| a | variable | Orbital separation — length metre |
| P | variable | Orbital period — time second |

















