law

law of conservation of angular momentum

The law of conservation of angular momentum states that the total angular momentum of a closed system remains constant.
22 related articles · 3 formulas · 3 who worked here

Description

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.

History

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.

How it works

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.

In practice

Attitude control of spacecraft (reaction wheels), sports spins, stabilization of pulsars.

Fun fact

A gyroscope, spun up to high speed, resists attempts to change its axis — navigation instruments operate on this principle.

Concept graph →

Formulas

$$I = \int r^2 dm$$
Moment of inertia measures mass distribution about axis.
What is in the formula
IvariableMoment of inertia about the axis — moment of inertia kilogram metre squared
rvariablePerpendicular distance from the axis to mass element — distance metre
dmvariableInfinitesimal mass element — mass kilogram
∫operatorIntegration over the entire body — integral operator
i=\frac{8π}{3}\int_0^rρ(r)r^4dr · 2607.02644
$$J^{\mu\nu\alpha}(x) = x^{\mu} T^{\nu\alpha}(x) - x^{\nu} T^{\mu\alpha}(x)$$
Local density of angular momentum in flat spacetime.
What is in the formula
J^{\mu\nu\alpha}variableAngular momentum density tensor — angular momentum density kilogram per metre per second
x^{\mu}variableSpacetime coordinate — position metre
x^{\nu}variableSpacetime coordinate — position metre
T^{\nu\alpha}variableStress-energy tensor component — stress energy tensor joule per cubic metre
T^{\mu\alpha}variableStress-energy tensor component — stress energy tensor joule per cubic metre
j^{μνα}(x)=x^{μ}t^{να}(x)-x^{ν}t^{μα}(x) · 2605.13557v1
$$\dot{J} = f(\dot{M}, M_1, M_2, a, P)$$
Rate of angular momentum loss in binary systems due to mass transfer.
What is in the formula
\dot{J}variableAngular momentum loss rate — angular momentum loss rate kilogram metre squared per second square
\dot{M}variableMass transfer rate — mass transfer rate kilogram per second
M_1variableMass of the primary star — mass kilogram
M_2variableMass of the secondary star — mass kilogram
avariableOrbital separation — length metre
PvariableOrbital period — time second
\dot{j}_{\rmml}=(α\dot{m}_{\rmtr}m_2^2+β\dot{m}_{\rmtr}m_1^2)(\frac{a}{m_1+m_2})^2\frac{2π}{p_{\rmorb}} · 2607.17552v1

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