Picard iteration

E121358

Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.

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Picard iteration canonical 1

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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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