<< series

Fourier Series

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# Orthogonality of Trigonometric Functions

\[ y = A\sin(\omega t + \varphi) \]

\[ y = A_0 + \sum_{n=1}^\infty A_n\sin(n\omega t + \varphi_n) = A_n\sin\varphi_n \cos n\omega t + A_n \cos\varphi_n\sin n\omega t \]

Let \(a_0/2 = A_0, a_n = A_n\sin\varphi_n, b_n = A_n\cos\varphi_n\), we have the function term series

\[ \frac{a_0}{2} + \sum_{k=1}^\infty(a_n\cos nx + b_n\sin nx) \]

The trigonometric function list

\[ 1, \cos x, \sin x, \cos 2x, \sin 2x, \ldots, \cos nx, \sin nx, \ldots \]

are orthogonal on \([-\pi, \pi]\), that is, the integral of multiplication of any of the two functions equal zero.

\[ \begin{align} & \int_{-\pi}^\pi \sin{k_1x}\cos{k_2x}\dx = 0 \\ & \int_{-\pi}^\pi \sin{k_1x}\sin{k_2x}\dx = 0 ~~~~ (k_1\neq k_2)\\ & \int_{-\pi}^\pi \cos{k_1x}\cos{k_2x}\dx = 0 ~~~~ (k_1\neq k_2)\\ \end{align} \]

These expressions can be easily proved by product-to-sum formula of trigonometric fucntionsq

Proof. \[ \begin{align} \int_{-\pi}^{\pi}\sin k_1x \cos k_2x &= \frac{1}{2}\int_{-\pi}^\pi [\sin(k_1+k_2)x + \sin(k_1-k_2)x]\dx \\ &= \frac{1}{2} \left.\left[-\frac{\cos(k_1+k_2)x}{k_1+k_2} -\frac{\cos(k_1-k_2)x}{k_1-k_2}\right]\right|_{-\pi}^{\pi} \\ &= 0 \end{align} \]

The other two expressions can be proved similarly.

On the contrary,

# Fourier Series

Assume the function with period \(2\pi\) can be expanded into trigonometric series or Fouries series \[ f(x) = \frac{a_0}{2} + \sum_{k=1}^\infty(a_k\cos kx + b_k\sin kx) \] The Fourier coefficients \(a_k, b_k\) are \[ \begin{align} & a_n = \frac{1}{\pi}\int_{-\pi}^{\pi}f(x)\cos nx \dx \\ & b_n = \frac{1}{\pi}\int_{-\pi}^{\pi}f(x)\sin nx \dx \end{align} \]

Example. Expand \(f(x)\) with period \(2\pi\) into its Fouries series, the expression on \([-\pi, \pi]\) is \[ f(x) = \left\{\begin{array}{ll}\begin{align} &-1, ~~~~ && -\pi \le x \lt 0 \\ &1, ~~~~ && 0 \le x \lt \pi \end{align}\end{array}\right. \]

\[ a_n = \frac{1}{\pi}\int_{-\pi}^{\pi}f(x)\cos nx \dx = \]