Orthogonality
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Definition
Two vectors $x$ and $y$ in an inner product space are orthogonal if their inner product is zero:
$$ \langle x, y \rangle = 0 $$We write $x \perp y$ to denote orthogonality.
For Functions
Two functions $f$ and $g$ are orthogonal if:
$$ \langle f, g \rangle = \int f(x) \overline{g(x)} \, dx = 0 $$Intuition
Orthogonal vectors are “perpendicular” — they point in completely independent directions. In the function space context, orthogonal functions have no “overlap” or “similarity.”
Examples
- In $\mathbb{R}^3$: $(1, 0, 0) \perp (0, 1, 0)$
- $\sin(nx)$ and $\sin(mx)$ are orthogonal on $[0, 2\pi]$ when $n \neq m$
- $\sin(nx)$ and $\cos(mx)$ are orthogonal on $[0, 2\pi]$ for all $n, m$
Orthonormal Basis
A set of vectors $\{e_1, e_2, \ldots\}$ is orthonormal if:
- $\langle e_i, e_j \rangle = 0$ for $i \neq j$ (orthogonal)
- $\langle e_i, e_i \rangle = 1$ for all $i$ (normalized)
Fourier series use orthonormal bases of sines and cosines.
Related Concepts
- Inner product — defines orthogonality
- Fourier transform — decomposes into orthogonal components
- basis — orthonormal bases simplify computations