Picard iteration
E121358
Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Picard iteration canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T1057157 — 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: Picard iteration Context triple: [local existence and uniqueness theorem, isProvedBy, Picard iteration]
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A.
Gauss–Seidel method
The Gauss–Seidel method is an iterative numerical technique used to solve systems of linear equations, particularly in large, sparse problems arising in scientific and engineering computations.
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B.
Euler’s method for numerical integration
Euler’s method for numerical integration is a simple first-order numerical procedure used to approximate solutions to ordinary differential equations by stepping forward in small increments.
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C.
Crank–Nicolson scheme
The Crank–Nicolson scheme is a finite difference method for numerically solving time-dependent partial differential equations, especially parabolic ones like the heat equation, known for its second-order accuracy and unconditional stability.
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D.
Aitken
Aitken is a Scottish-origin surname notably borne by Max Aitken, 1st Baron Beaverbrook, a prominent Canadian-British newspaper magnate and politician.
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E.
Euler–Maruyama method
The Euler–Maruyama method is a basic time-stepping scheme for numerically approximating solutions to stochastic differential equations, widely used in simulations of systems with noise such as Langevin dynamics.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Picard iteration Target entity description: Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.
-
A.
Gauss–Seidel method
The Gauss–Seidel method is an iterative numerical technique used to solve systems of linear equations, particularly in large, sparse problems arising in scientific and engineering computations.
-
B.
Euler’s method for numerical integration
Euler’s method for numerical integration is a simple first-order numerical procedure used to approximate solutions to ordinary differential equations by stepping forward in small increments.
-
C.
Crank–Nicolson scheme
The Crank–Nicolson scheme is a finite difference method for numerically solving time-dependent partial differential equations, especially parabolic ones like the heat equation, known for its second-order accuracy and unconditional stability.
-
D.
Aitken
Aitken is a Scottish-origin surname notably borne by Max Aitken, 1st Baron Beaverbrook, a prominent Canadian-British newspaper magnate and politician.
-
E.
Euler–Maruyama method
The Euler–Maruyama method is a basic time-stepping scheme for numerically approximating solutions to stochastic differential equations, widely used in simulations of systems with noise such as Langevin dynamics.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
fixed-point iteration method
ⓘ
method for ordinary differential equations ⓘ numerical method ⓘ successive approximation method ⓘ |
| advantage | provides rigorous existence and uniqueness proof ⓘ |
| appliesTo | initial value problems for ordinary differential equations ⓘ |
| assumes |
boundedness of f on the considered domain
ⓘ
complete metric space of candidate functions ⓘ |
| basedOn | Banach fixed-point theorem ⓘ |
| category |
analytical method in differential equations
ⓘ
constructive proof technique ⓘ |
| constructs | solution as limit of iterative sequence ⓘ |
| contrastWith |
Euler’s method for numerical integration
ⓘ
surface form:
Euler method
Runge–Kutta methods ⓘ |
| convergesTo | unique fixed point of the associated integral operator ⓘ |
| convergesUnderCondition |
Lipschitz condition on the function f(t,y)
ⓘ
sufficiently small time interval ⓘ |
| definesSequence | sequence of approximate solutions ⓘ |
| ensures |
continuous dependence of solutions on initial data under Lipschitz conditions
ⓘ
uniform convergence on compact subintervals under standard hypotheses ⓘ |
| firstApproximation | constant function equal to initial value y0 ⓘ |
| formulatedAs | integral equation equivalent to the differential equation ⓘ |
| guarantees |
local existence of solution
ⓘ
local uniqueness of solution ⓘ |
| historicalPeriod | late 19th century ⓘ |
| iterationFormula | y_{n+1}(t) = y0 + ∫_{t0}^{t} f(s, y_n(s)) ds ⓘ |
| limitation | may be computationally expensive for practical numerical use ⓘ |
| mathematicalDomain |
analysis
ⓘ
ordinary differential equations ⓘ |
| namedAfter | Charles Émile Picard ⓘ |
| operatorType | integral operator ⓘ |
| proofRole | constructive proof of Picard–Lindelöf theorem ⓘ |
| provides | successive approximations converging to exact solution ⓘ |
| relatedTo |
local existence and uniqueness theorem
ⓘ
surface form:
Picard–Lindelöf theorem
contraction mapping principle ⓘ fixed-point theory ⓘ |
| requires |
Lipschitz continuity of the right-hand side of the differential equation
ⓘ
continuity of the right-hand side of the differential equation ⓘ |
| typicalProblemForm | y'(t) = f(t,y(t)), y(t0) = y0 ⓘ |
| typicalSpace | space of continuous functions on a closed interval ⓘ |
| usedBy |
applied mathematicians
ⓘ
engineers modeling dynamical systems ⓘ mathematicians studying initial value problems ⓘ |
| usedFor |
constructing solutions to ordinary differential equations
ⓘ
proving existence of solutions to ordinary differential equations ⓘ proving uniqueness of solutions to ordinary differential equations ⓘ |
| usedIn |
numerical approximation of solutions to differential equations
ⓘ
theoretical analysis of differential equations ⓘ |
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Subject: Picard iteration Description of subject: Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.
Referenced by (1)
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