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FredholmIntegralEquationOfTheFirstKind
Given a Fredholm integral equation of the first kind:
where (K(x, y)) is the kernel, (\phi(y)) is the unknown function, and (f(x)) is a known function.
The approach involves projecting a set of functions onto the kernel (K(x, y)), calculating weights by the inner product:
where ({\psi_i}) is a set of orthogonal polynomials converging point-wise to the reproducing kernel.
The goal is to achieve uniform convergence of the sequence of polynomials to the solution, represented as:
ensuring that (\lim_{n \to \infty} \phi_n(x) = \phi(x)) uniformly.
The eigenfunctions can be derived by substituting the basis into the integral equation:
applying Fubini's theorem to swap summation and integration, leading to term-wise integration.
The variational method minimizes the functional:
where the solution (\phi) minimizes (J[\phi]) over an appropriate function space.
Galerkin's method seeks to solve:
by ensuring the residual is orthogonal to the space spanned by the chosen basis ({\psi_i}):
The approach combines the principles of the variational method and Galerkin's method, utilizing a point-wise converging set of polynomials, ensuring uniform convergence and deriving eigenfunctions through a sophisticated application of functional analysis and spectral theory.