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Advanced Linear Algebra, Lecture 5.2: Orthogonality
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Advanced Linear Algebra, Lecture 5.2: Orthogonality
Two vectors are orthogonal if their inner product is zero. This is the analogue of the concept of being perpendicular in Euclidean space to a general inner product space. Orthogonal bases are particular nice, because the coefficients of any linear combination of the basis vectors are simply a projection, and given by the formula a_i = (v, x_i)/(x_i,x_i). We derive this formula, do some example of what orthogonality means in a number of inner product vector spaces, including applications to Fourier series, and Sturm-Liouville theory, where the Legendre and Chebyshev polynomials arise. Our examples of these infinite dimensional functional spaces are meant to just be a tour, highlighting the diversity of applications of orthogonality in inner product spaces within math, science, and engineering.
Two vectors are orthogonal if their inner product is zero. This is the analogue of the concept of being perpendicular in Euclidean space to a general inner product space. Orthogonal bases are particular nice, because the coefficients of any linear combination of the basis vectors are simply a projection, and given by the formula a_i = (v, x_i)/(x_i,x_i). We derive this formula, do some example of what orthogonality means in a number of inner product vector spaces, including applications to Fourier series, and Sturm-Liouville theory, where the Legendre and Chebyshev polynomials arise. Our examples of these infinite dimensional functional spaces are meant to just be a tour, highlighting the diversity of applications of orthogonality in inner product spaces within math, science, and engineering.