Kovalevskaya integral

E662759

The Kovalevskaya integral is an additional conserved quantity that makes the motion of the Kovalevskaya top exactly integrable in classical rigid body dynamics.

All labels observed (1)

Label Occurrences
Kovalevskaya integral canonical 1

How this entity was disambiguated

Statements (31)

Predicate Object
instanceOf conserved quantity ⓘ
first integral ⓘ
integral of motion ⓘ
appliesTo Kovalevskaya top ⓘ
associatedWith Kovalevskaya exponents and special inertia relations ⓘ
category conservation laws in mechanics ⓘ
contributesTo complete set of independent integrals for the Kovalevskaya top ⓘ
dependsOn angular velocities of the rigid body ⓘ
direction cosines of the gravity vector ⓘ
ensures Liouville integrability of the Kovalevskaya top ⓘ
field classical mechanics ⓘ
integrable systems ⓘ
rigid body dynamics ⓘ
historicalContext discovered in the 19th century ⓘ
independence functionally independent of energy and momentum integrals ⓘ
mathematicalForm quartic polynomial in phase-space variables (up to canonical transformations) ⓘ
namedAfter Sofya Kovalevskaya ⓘ
linked to: Sofia Kovalevskaya
relatedTo Euler–Poisson equations ⓘ
Kovalevskaya case of a heavy rigid body about a fixed point ⓘ
linked to: Kovalevskaya top
requiresCondition specific ratio of principal moments of inertia of the rigid body ⓘ
roleInSystem additional conserved quantity ⓘ
ensures complete integrability ⓘ
studiedIn Hamiltonian mechanics ⓘ
theory of integrable Hamiltonian systems ⓘ
timeDerivative zero along solutions of the Kovalevskaya top equations ⓘ
togetherWith area integral ⓘ
energy integral ⓘ
geometric integral ⓘ
typeOfConservation nontrivial polynomial integral ⓘ
usedIn analysis of exact solutions for the Kovalevskaya top ⓘ
separation of variables for the Kovalevskaya top ⓘ

How these facts were elicited

Referenced by (1)

Full triples — surface form annotated when it differs from this entity's canonical label.

Kovalevskaya top → hasIntegralOfMotion → Kovalevskaya integral ⓘ