brachistochrone problem
E270049
The brachistochrone problem is a famous challenge in the calculus of variations that asks for the curve along which a particle will descend between two points in the shortest time under gravity, whose solution is a cycloid.
All labels observed (1)
| Label | Occurrences |
|---|---|
| brachistochrone problem canonical | 2 |
How this entity was disambiguated
This entity first appeared as the object of triple T2467334 — 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: brachistochrone problem Context triple: [Johann Bernoulli, notableWork, brachistochrone problem]
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A.
Euler–Lagrange equation
The Euler–Lagrange equation is a fundamental differential equation in the calculus of variations that provides the condition for a function to make a functional stationary, forming the basis of Lagrangian mechanics and many physical theories.
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B.
Hamilton–Jacobi equation
The Hamilton–Jacobi equation is a fundamental partial differential equation in classical mechanics that reformulates dynamics in terms of a generating function, providing a powerful bridge to quantum mechanics and modern analytical methods.
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C.
Fermat’s principle of least time
Fermat’s principle of least time is a fundamental variational principle in optics stating that light follows the path that takes the least time, from which many laws of geometrical optics can be derived.
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D.
principle of least action
The principle of least action is a fundamental concept in physics stating that the path taken by a physical system between two states is the one for which a specific quantity called the action is minimized (or made stationary), forming the basis of Lagrangian and Hamiltonian mechanics.
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E.
d’Alembert’s principle
d’Alembert’s principle is a fundamental concept in classical mechanics that reformulates Newton’s laws to analyze the motion of systems by introducing inertial forces so they can be treated as if in static equilibrium.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: brachistochrone problem Target entity description: The brachistochrone problem is a famous challenge in the calculus of variations that asks for the curve along which a particle will descend between two points in the shortest time under gravity, whose solution is a cycloid.
-
A.
Euler–Lagrange equation
The Euler–Lagrange equation is a fundamental differential equation in the calculus of variations that provides the condition for a function to make a functional stationary, forming the basis of Lagrangian mechanics and many physical theories.
-
B.
Hamilton–Jacobi equation
The Hamilton–Jacobi equation is a fundamental partial differential equation in classical mechanics that reformulates dynamics in terms of a generating function, providing a powerful bridge to quantum mechanics and modern analytical methods.
-
C.
Fermat’s principle of least time
Fermat’s principle of least time is a fundamental variational principle in optics stating that light follows the path that takes the least time, from which many laws of geometrical optics can be derived.
-
D.
principle of least action
The principle of least action is a fundamental concept in physics stating that the path taken by a physical system between two states is the one for which a specific quantity called the action is minimized (or made stationary), forming the basis of Lagrangian and Hamiltonian mechanics.
-
E.
d’Alembert’s principle
d’Alembert’s principle is a fundamental concept in classical mechanics that reformulates Newton’s laws to analyze the motion of systems by introducing inertial forces so they can be treated as if in static equilibrium.
- F. None of above. chosen
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
mathematical problem
ⓘ
problem in the calculus of variations ⓘ |
| application |
design of roller coaster profiles
ⓘ
optimal control theory ⓘ time-optimal motion planning ⓘ |
| asksFor | curve of fastest descent under gravity between two points ⓘ |
| assumes |
motion constrained to a vertical plane
ⓘ
no friction ⓘ particle starts from rest ⓘ particle treated as point mass ⓘ uniform gravitational field ⓘ |
| constraintType | holonomic constraint to a curve in a plane ⓘ |
| field |
calculus of variations
ⓘ
classical mechanics ⓘ mathematical physics ⓘ |
| generalization |
brachistochrone in non-uniform gravitational fields
ⓘ
relativistic brachistochrone problem ⓘ |
| historicalContext | early problem in the development of the calculus of variations ⓘ |
| mathematicalFormulation | minimization of a time functional over admissible curves ⓘ |
| nameEtymology | from Greek "brachistos" meaning shortest and "chronos" meaning time ⓘ |
| objectiveFunction | time of travel along the curve under gravity ⓘ |
| posedBy | Johann Bernoulli ⓘ |
| publishedIn | Acta Eruditorum ⓘ |
| receivedSolutionsFrom |
Gottfried Wilhelm Leibniz
ⓘ
Guillaume de l’Hôpital ⓘ
surface form:
Guillaume de l'Hôpital
Isaac Newton ⓘ Jakob Bernoulli ⓘ
surface form:
Jacob Bernoulli
Tschirnhaus ⓘ |
| relatedConcept |
Euler–Lagrange equation
ⓘ
Fermat’s principle of least time ⓘ
surface form:
Fermat's principle
geodesic ⓘ principle of least action ⓘ tautochrone problem ⓘ |
| solutionCurve | cycloid ⓘ |
| solutionFamily | one-parameter family of cycloidal arcs through given endpoints ⓘ |
| solutionProperty |
gives minimum time of descent
ⓘ
not a circular arc ⓘ not a straight line ⓘ |
| standardExampleIn |
advanced mechanics textbooks
ⓘ
introductory courses on calculus of variations ⓘ |
| teachesConcept |
difference between shortest path and quickest path
ⓘ
variational extremals may be non-intuitive curves ⓘ |
| typicalAssumption | fixed endpoints with lower point vertically below upper point or horizontally displaced ⓘ |
| usesMethod |
Euler–Lagrange equation
ⓘ
surface form:
Euler–Lagrange differential equation
Snell's law analogy ⓘ |
| usesPrinciple | conservation of mechanical energy ⓘ |
| yearPosed | 1696 ⓘ |
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Subject: brachistochrone problem Description of subject: The brachistochrone problem is a famous challenge in the calculus of variations that asks for the curve along which a particle will descend between two points in the shortest time under gravity, whose solution is a cycloid.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.