concept

angular momentum

Angular momentum is a conserved quantity representing rotational motion in physics, from quantum to cosmic scales.
19 related articles · 6 formulas · 2 who worked here

Description

When you spin on a chair with your legs stretched out and then pull them in, you start spinning faster. This is because you have "rotational stubbornness" — angular momentum. The farther the mass is from the axis of rotation, the stronger the "stubbornness," but if it's pulled in, the rotation speeds up. Ice skaters use this for fast pirouettes!

History

The concept of angular momentum dates back to Kepler's law of areas (1609), which was explained by Newton and later expressed as conservation of angular momentum. Leonard Euler in the 18th century developed the mathematical apparatus for rotational motion. Henri Poincaré in the late 19th century explored the connection between conservation laws and symmetries. In quantum mechanics, angular momentum was quantized and given an interpretation in terms of operator eigenvalues. In black holes, its role is described by Kerr solutions, and in black hole thermodynamics, by the works of Bekenstein and Hawking.

How it works

In classical mechanics, angular momentum is conserved in the absence of an external torque. For a rigid body, it is expressed as L = I ω, where I is the inertia tensor. In quantum mechanics, there are operators for orbital (L̂) and spin (Ŝ) angular momentum with discrete values, e.g., L = ħ√(l(l+1)). In general relativity, a rotating black hole is described by the Kerr metric, where the spin parameter a = J/Mc introduces frame-dragging effects. Conservation of angular momentum is tied to the isotropy of space through Noether's theorem, and for black holes, to the generalized laws of mechanics.

Fun fact

Do you know why a bicycle doesn't fall when it moves? The wheels are spinning, and their angular momentum helps maintain balance. Even a falling cat, by twisting, uses its angular momentum to land on its feet!

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Formulas

$$J^{\mu\nu\alpha}(x) = x^{\mu} T^{\nu\alpha}(x) - x^{\nu} T^{\mu\alpha}(x)$$
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
$$L_{\text{sd}} = -I \Omega \dot{\Omega}$$
Rotational energy loss rate equals moment of inertia times angular velocity times its derivative.
What is in the formula
Ivariablemoment of inertia — moment of inertia kilogram metre squared
Ωvariableangular velocity — angular velocity radian per second
Ω̇variabletime derivative of angular velocity — angular acceleration radian per second squared
l_{{spin-down}}=-4π^2i\frac{\dot{p}}{p^3} · 2606.29653
l_{\rmsd}=\frac{4π^2i\dot{p}}{p^3} · 2607.03848v1
$$I = \int r^2 dm$$
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
$$j^2 = a(1-e^2)$$
Specific angular momentum squared in Keplerian orbits.
What is in the formula
jvariablespecific angular momentum — specific angular momentum metre squared per second
avariablesemi-major axis — semi major axis metre
evariableorbital eccentricity — eccentricity
j^2=a(1-e^2) · 2607.16406v1
$$\dot{J} = f(\dot{M}, M_1, M_2, a, P)$$
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
$$I = k M R^2$$
Moment of inertia for spherical objects with mass distribution.
What is in the formula
IvariableMoment of inertia — moment of inertia kilogram metre squared
kvariableDimensionless shape factor
MvariableMass of the sphere — mass kilogram
RvariableRadius of the sphere — radius metre
i\approx\frac{2}{5}(1+y)mr^2 · 2607.17609v1

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