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Orthogonal Functions and Fourier Series

Orthogonal Functions and Fourier Series. Vector Spaces. Set of vectors Closed under the following operations Vector addition: v 1 + v 2 = v 3 Scalar multiplication: s v 1 = v 2 Linear combinations: Scalars come from some field F e.g. real or complex numbers Linear independence

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Orthogonal Functions and Fourier Series

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  1. Orthogonal Functions and Fourier Series University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  2. Vector Spaces • Set of vectors • Closed under the following operations • Vector addition: v1 + v2 = v3 • Scalar multiplication: sv1 = v2 • Linear combinations: • Scalars come from some field F • e.g. real or complex numbers • Linear independence • Basis • Dimension University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  3. Vector Space Axioms • Vector addition is associative and commutative • Vector addition has a (unique) identity element (the 0 vector) • Each vector has an additive inverse • So we can define vector subtraction as adding an inverse • Scalar multiplication has an identity element (1) • Scalar multiplication distributes over vector addition and field addition • Multiplications are compatible (a(bv)=(ab)v) University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  4. Coordinate Representation • Pick a basis, order the vectors in it, then all vectors in the space can be represented as sequences of coordinates, i.e. coefficients of the basis vectors, in order. • Example: • Cartesian 3-space • Basis: [i j k] • Linear combination: xi + yj + zk • Coordinate representation: [x y z] University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  5. Functions as vectors • Need a set of functions closed under linear combination, where • Function addition is defined • Scalar multiplication is defined • Example: • Quadratic polynomials • Monomial (power) basis: [x2x1] • Linear combination: ax2 + bx + c • Coordinate representation: [a b c] University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  6. Metric spaces • Define a (distance)metric s.t. • d is nonnegative • d is symmetric • Indiscernibles are identical • The triangle inequality holds University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  7. Normed spaces • Define the length or norm of a vector • Nonnegative • Positive definite • Symmetric • The triangle inequality holds • Banach spaces – normed spaces that are complete (no holes or missing points) • Real numbers form a Banach space, but not rational numbers • Euclidean n-space is Banach University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  8. Norms and metrics • Examples of norms: • p norm: • p=1 manhattan norm • p=2 euclidean norm • Metric from norm • Norm from metric if • d is homogeneous • d is translation invariant then University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  9. Inner product spaces • Define [inner, scalar, dot] product (for real spaces)s.t. • For complex spaces: • Induces a norm: University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  10. Some inner products • Multiplication in R • Dot product in Euclidean n-space • For real functions over domain [a,b] • For complex functions over domain [a,b] • Can add nonnegative weight function University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  11. Hilbert Space • An inner product space that is complete wrt the induced norm is called a Hilbert space • Infinite dimensional Euclidean space • Inner product defines distances and angles • Subset of Banach spaces University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  12. Orthogonality • Two vectors v1 and v2 are orthogonal if • v1 and v2 are orthonormal if they are orthogonal and • Orthonormal set of vectors (Kronecker delta) University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  13. Examples • Linear polynomials over [-1,1] (orthogonal) • B0(x) = 1, B1(x) = x • Is x2 orthogonal to these? • Is orthogonal to them? (Legendre) University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  14. Fourier series Cosine series University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  15. Fourier series • Sine series University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  16. Fourier series • Complete series • Basis functions are orthogonal but not orthonormal • Can obtain an and bn by projection University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

  17. Fourier series • Similarly for bk University of Texas at Austin CS384G - Computer Graphics Fall 2008 Don Fussell

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