Math 2.0

Integral equations Theoretical approximation of solutions Theorem

Convergence of approximations for second-kind equations

Builds on Banach spaceCompact operatorProjection method for integral equationsIntegral equation of the second kindStrong operator topology

Statement

Let XX be a Banach space, let K ⁣:X→XK \colon X \to X be a compact operator such that I−KI - K is injective, and let f∈Xf \in X. Let φ∈X\varphi \in X be the solution of φ−Kφ=f\varphi - K\varphi = f. Let Pn ⁣:X→XP_n \colon X \to X be bounded linear projections onto finite-dimensional subspaces XnX_n such that Pnψ→ψP_n \psi \to \psi for every ψ∈X\psi \in X. Then there is n0n_0 such that for every n≥n0n \ge n_0 the projection method equation φn−PnKφn=Pnf\varphi_n - P_n K \varphi_n = P_n f has a unique solution φn∈X\varphi_n \in X, which lies in XnX_n. Moreover there is a constant MM, independent of nn and ff, such that ∥φn−φ∥≤M∥Pnφ−φ∥for all n≥n0,\norm{\varphi_n - \varphi} \le M \norm{P_n \varphi - \varphi} \quad \text{for all } n \ge n_0, and in particular φn→φ\varphi_n \to \varphi.

Remarks

The solution φ\varphi exists because, for compact KK, injectivity of I−KI - K implies that I−KI - K is invertible with bounded inverse (Riesz theory, the Fredholm alternative). Since Pnψ→ψP_n \psi \to \psi for each ψ\psi, the norms ∥Pn∥\norm{P_n} are bounded by the uniform boundedness principle, so the convergence is uniform on compact sets. The set {Kψ:∥ψ∥≤1}\set{K\psi : \norm{\psi} \le 1} is relatively compact, hence ∥PnK−K∥→0\norm{P_n K - K} \to 0. A perturbation argument then shows that I−PnKI - P_n K is invertible for large nn, with ∥(I−PnK)−1∥≤M\norm{(I - P_n K)^{-1}} \le M. Finally (I−PnK)(φn−φ)=Pnφ−φ(I - P_n K)(\varphi_n - \varphi) = P_n \varphi - \varphi, which gives the error bound; and if φn−PnKφn=Pnf\varphi_n - P_nK\varphi_n = P_n f then φn=Pn(f+Kφn)∈Xn\varphi_n = P_n(f + K\varphi_n) \in X_n.

Example: for a continuous kernel on [a,b][a, b], collocation with piecewise linear interpolation on grids with mesh tending to 00 satisfies the hypothesis in C[a,b]C[a, b], since Pnψ→ψP_n \psi \to \psi uniformly for continuous ψ\psi. The error is then of the order of the interpolation error of the exact solution, for instance O(h2)O(h^2) for a twice continuously differentiable φ\varphi and mesh size hh.

The hypothesis of pointwise convergence Pnψ→ψP_n \psi \to \psi is needed. For collocation with polynomial interpolation at equidistant points in C[a,b]C[a, b] it fails, since the norms of the interpolation operators grow without bound, and the theorem gives nothing.

Going deeper

For a student

The key step is that a compact operator turns pointwise convergence of PnP_n into norm convergence of PnKP_n K. This is why second-kind equations with compact KK are so well suited to numerical methods, in contrast to first-kind equations, which are ill-posed. In a Hilbert space with orthogonal projections, this gives the convergence of the Galerkin method for second-kind equations. For the Nyström method, KK is replaced by quadrature operators KnK_n that do not converge in norm, and the same conclusion needs collectively compact operator approximation.

Reading path

To understand this page from the ground up, read these 6 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
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  1. Banach space concept
  2. Compact operator concept
  3. Integral equation of the second kind concept
  4. Projection method for integral equations concept
  5. Strong operator topology concept
  6. Convergence of approximations for second-kind equations statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Fredholm_integral_equation
About this page
TagH6KS0E9MF5
URIm2://H6KS0E9MF5
Kindstatement, theorem
WritingW0 stub
MSC45L05, 65R20, 47A58
StatusThis copy of the site has no build data. Run m2 status H6KS0E9MF5.
AboutProjection method for integral equations, Integral equation of the second kind
UsesBanach space, Compact operator, Projection method for integral equations, Integral equation of the second kind, Strong operator topology

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