Fourier Series/Square Wave/Special Cases
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Special Cases of Fourier Series for Square Wave
Unit Half Interval
Let $\map S x$ be the square wave defined on the real numbers $\R$ as:
- $\forall x \in \R: \map S x = \begin {cases}
1 & : x \in \openint 0 1 \\ -1 & : x \in \openint {-1} 0 \\ \map S {x + 2} & : x < -1 \\ \map S {x - 2} & : x > +1 \end {cases}$
Then its Fourier series can be expressed as:
\(\ds \map S x\) | \(\sim\) | \(\ds \frac 4 \pi \sum_{r \mathop = 0}^\infty \frac 1 {2 r + 1} {\sin \pi x}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac 4 \pi \paren {\sin \pi x + \dfrac {\sin 3 \pi x} 3 + \dfrac {\sin 5 \pi x} 5 + \dotsb}\) |
Half Interval $\pi$
Let $\map S x$ be the square wave defined on the real numbers $\R$ as:
- $\forall x \in \R: \map S x = \begin {cases}
1 & : x \in \openint 0 \pi \\ -1 & : x \in \openint {-\pi} 0 \\ \map S {x + 2 \pi} & : x < -\pi \\ \map S {x - 2 \pi} & : x > +\pi \end {cases}$
Then its half-range Fourier sine series can be expressed as:
\(\ds \map S x\) | \(\sim\) | \(\ds \frac 4 \pi \sum_{r \mathop = 0}^\infty \frac 1 {2 r + 1} {\sin x}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac 4 \pi \paren {\sin x + \dfrac {\sin 3 x} 3 + \dfrac {\sin 5 x} 5 + \dotsb}\) |