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chebintconv.md

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@@ -87,6 +87,7 @@ Thus $f^{(\nu)}$ of bounded variation implies that the convergence is at an alge
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:::{prf:example} Piecewise continuous function
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:label: ex:pwctschebint
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For $\nu = 0$, e.g., $f(x) = \textrm{sign}(x)$, we cannot hope for convergence since polynomials are continuous and sign function is not.
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Even the projections do not converge, since

fourier.md

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@@ -38,7 +38,7 @@ For results on convergence of Fourier series, see
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## Fourier series
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Let $f : [-\pi,\pi] \to \re$ be a function which is extended periodically to the whole real line. The Fourier series is defined as
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Let $f : [-\pi,\pi] \to \re$ be a function which is extended periodically to the whole real line. The Fourier series of $f$ is defined as
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$$
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Sf(x) = a_0 + \sum_{k=1}^\infty [ a_k \cos(k x) + b_k \sin(k x) ]
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b_k &= \frac{1}{\pi} \int_{-\pi}^\pi f(x) \sin(k x) \ud x, \qquad k=1, 2, \ldots
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$$
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Due to periodicity $k$ only takes integer values.
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Due to periodicity of $f$, the wavenumber $k$ only takes integer values.
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The Fourier series can be written as
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Its Fourier coefficients are
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$$
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\label{eq:ftcinper}
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\hat f_k = \frac{2}{\pi(1 - 4 k^2)}, \qquad |\hat f_k| = \order{\frac{1}{k^2}}, \qquad |k| \to \infty
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$$
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compute_fk()
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```
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This agrees with the Fourier transform shown in equation [](#eq:ftcinper).
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As $n$ increases, we see that the errors do not decrease around the discontinuities and there is no convergence in maximum norm, but there is convergence in 2-norm as stated in Part (1) of [](#thm:fserconv).
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We have observed this kind of Gibbs oscillations when we interpolate a discontinuous function with polynomials.
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We have observed this kind of Gibbs oscillations when we interpolate a discontinuous function with polynomials, see Example [](#ex:pwctschebint).
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Moreover, it looks like there is pointwise convergence away from the discontinuities, and this is the case, see next Theorem.
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intro.md

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@@ -207,6 +207,6 @@ with $p$ as large as possible. Both of these properties will imply convergence o
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**Algorithms**: Efficient implementation of numerical methods in a working code is very important. E.g., trigonometic interpolation would be costly if implemented in a naive way, while FFT provides a fast implementation.
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:::{seealso}
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1. L. N. Trefethen, Numerical Analysis
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1. L. N. Trefethen, The definition of numerical analysis
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1. [L. N. Trefethen, Numerical Analysis](https://people.maths.ox.ac.uk/trefethen/NAessay.pdf)
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1. [L. N. Trefethen, The definition of numerical analysis](https://people.maths.ox.ac.uk/trefethen/publication/PDF/1992_55.pdf)
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