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
This entity first appeared as the object of triple T7419954 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Kovalevskaya integral Context triple: [Kovalevskaya top, hasIntegralOfMotion, Kovalevskaya integral]
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A.
Kovalevskaya top
The Kovalevskaya top is a famous integrable case of the motion of a rigid body about a fixed point in classical mechanics, discovered and analyzed by mathematician Sofia Kovalevskaya.
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B.
Jacobi integral
The Jacobi integral is a conserved quantity in celestial mechanics and dynamical systems that simplifies the analysis of motion in rotating reference frames, particularly in the restricted three-body problem.
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C.
Liouville–Arnold theorem
The Liouville–Arnold theorem is a fundamental result in Hamiltonian mechanics that guarantees the integrability of a system with sufficiently many conserved quantities and describes its motion as quasi-periodic on invariant tori in phase space.
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D.
Kolmogorov–Arnold–Moser theory
Kolmogorov–Arnold–Moser theory is a fundamental result in dynamical systems that explains the persistence of quasi-periodic motions in nearly integrable Hamiltonian systems under small perturbations.
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E.
Cauchy–Kovalevskaya theorem
The Cauchy–Kovalevskaya theorem is a fundamental result in partial differential equations that guarantees the existence and uniqueness of analytic solutions to certain initial value problems under appropriate analyticity conditions.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Kovalevskaya integral Target entity description: The Kovalevskaya integral is an additional conserved quantity that makes the motion of the Kovalevskaya top exactly integrable in classical rigid body dynamics.
-
A.
Kovalevskaya top
The Kovalevskaya top is a famous integrable case of the motion of a rigid body about a fixed point in classical mechanics, discovered and analyzed by mathematician Sofia Kovalevskaya.
-
B.
Jacobi integral
The Jacobi integral is a conserved quantity in celestial mechanics and dynamical systems that simplifies the analysis of motion in rotating reference frames, particularly in the restricted three-body problem.
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C.
Liouville–Arnold theorem
The Liouville–Arnold theorem is a fundamental result in Hamiltonian mechanics that guarantees the integrability of a system with sufficiently many conserved quantities and describes its motion as quasi-periodic on invariant tori in phase space.
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D.
Kolmogorov–Arnold–Moser theory
Kolmogorov–Arnold–Moser theory is a fundamental result in dynamical systems that explains the persistence of quasi-periodic motions in nearly integrable Hamiltonian systems under small perturbations.
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E.
Cauchy–Kovalevskaya theorem
The Cauchy–Kovalevskaya theorem is a fundamental result in partial differential equations that guarantees the existence and uniqueness of analytic solutions to certain initial value problems under appropriate analyticity conditions.
- F. None of above. chosen
Statements (31)
| Predicate | Object |
|---|---|
| instanceOf |
conserved quantity
ⓘ
first integral ⓘ integral of motion ⓘ |
| appliesTo | Kovalevskaya top NERFINISHED ⓘ |
| 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 NERFINISHED ⓘ |
| relatedTo |
Euler–Poisson equations
NERFINISHED
ⓘ
Kovalevskaya case of a heavy rigid body about a fixed point NERFINISHED ⓘ |
| requiresCondition | specific ratio of principal moments of inertia of the rigid body ⓘ |
| roleInSystem |
additional conserved quantity
ⓘ
ensures complete integrability ⓘ |
| studiedIn |
Hamiltonian mechanics
NERFINISHED
ⓘ
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
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Subject: Kovalevskaya integral Description of subject: The Kovalevskaya integral is an additional conserved quantity that makes the motion of the Kovalevskaya top exactly integrable in classical rigid body dynamics.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.