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Calculus of variations and optimal control; optimization Definition

Admissible function

Builds on Integral functional with a Lagrangian densityContinuously differentiable function

Definition

Let a<ba < b and A,B∈ℝA, B \in \R, and let J(y)=∫abL(x,y,y′) dxJ(y) = \int_a^b L(x, y, y') \, dx be an integral functional with a continuous Lagrangian L ⁣:[a,b]×ℝ×ℝ→ℝL \colon [a, b] \times \R \times \R \to \R. In the fixed-endpoint problem for JJ, a function y ⁣:[a,b]→ℝy \colon [a, b] \to \R is admissible if:

  1. y∈C1([a,b])y \in C^1([a, b]), that is, yy is continuously differentiable on [a,b][a, b];
  2. y(a)=Ay(a) = A;
  3. y(b)=By(b) = B.

The set 𝒜\mathcal{A} of admissible functions is the admissible class. More generally, the admissible class of a variational problem is the set of functions in the domain of the functional that satisfy all its constraints. Its elements are the admissible functions.

Remarks

Example: for a=0a = 0, b=1b = 1, A=0A = 0, B=1B = 1, the function y(x)=x2y(x) = x^2 is admissible: it is C1C^1, y(0)=0y(0) = 0 and y(1)=1y(1) = 1. Non-example: for a=0a = 0, b=1b = 1, A=B=1A = B = 1, the function y(x)=∣x−1/2∣+1/2y(x) = \abs{x - 1/2} + 1/2 satisfies y(0)=y(1)=1y(0) = y(1) = 1 but is not differentiable at 1/21/2, so it fails clause 1. Many texts use the larger class of piecewise C1C^1 functions, which admits such broken curves. If yy is admissible and η∈C1([a,b])\eta \in C^1([a, b]) has η(a)=η(b)=0\eta(a) = \eta(b) = 0, then y+tηy + t\eta is admissible for every t∈ℝt \in \R; such η\eta are the admissible variations.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Calculus_of_variations
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Kinddefinition
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MSC49K05, 49J05
DefinesAdmissible function
UsesIntegral functional with a Lagrangian density, Continuously differentiable function

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