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Gaussian integration

The integral over a finite interval of a function $ w(t)f(t) $ for an arbitrary function $ f $ with a non-negative weight function $ w(t) $ can be approximated by integrating its approximation by Lagrange polynomials:

$\displaystyle \int\limits _{a}^{b}w(t)f(t)dt$ $\displaystyle \approx$ $\displaystyle \int\limits _{a}^{b}w(t)\sum ^{n}_{j=1}\prod ^{n}_{\begin{array}{...
..._{i}}f(t_{j})\mathrm{d}t+\int\limits _{a}^{b}w(t)v(t)f[t_{1},\ldots ,t_{n},t]dt$  
  $\displaystyle =$ $\displaystyle \sum ^{n}_{j=1}\int\limits _{a}^{b}w(t)\prod ^{n}_{\begin{array}{...
...1\\
i\neq j
\end{array}}\frac{t-t_{i}}{t_{j}-t_{i}}\mathrm{d}t\, f(t_{j})+R(f)$  
  $\displaystyle =$ $\displaystyle \sum _{j=1}^{n}A_{j}f(t_{j})+R(f)$ (12)

where $ v(t)=\prod\limits _{i=1}^{n}(t-t_{i}) $. Thus the constant coefficients

$\displaystyle A_{j}=\int\limits _{a}^{b}w(t)\prod ^{n}_{\begin{array}{c}
i=1\\
i\neq j
\end{array}}\frac{t-t_{i}}{t_{j}-t_{i}}\mathrm{d}t$

are found which are used for the approximation of the integral.



Subsections

Andreas Markmann 2003-10-22