🧚🏽‍♀️Abstract Linear Algebra I Unit 8 – Inner Products and Orthogonality

Inner products and orthogonality are fundamental concepts in linear algebra, extending geometric ideas to abstract vector spaces. These tools allow us to define angles, lengths, and perpendicularity, enabling powerful techniques like orthogonal projections and the Gram-Schmidt process. These concepts have wide-ranging applications, from least-squares approximations to quantum mechanics. Understanding inner products and orthogonality provides a solid foundation for advanced topics in linear algebra and its applications in various fields of mathematics and science.

Key Concepts and Definitions

  • Inner product is a generalization of the dot product that allows us to define angles and lengths in abstract vector spaces
  • Orthogonality refers to two vectors being perpendicular or at right angles to each other
    • Orthogonal vectors have an inner product of zero
  • Norm of a vector is a measure of its length or magnitude in a vector space
    • Induced by the inner product as v,v\sqrt{\langle v, v \rangle}
  • Orthonormal set is a collection of vectors that are both orthogonal to each other and have unit norm (length 1)
  • Orthogonal projection is the process of finding the closest point in a subspace to a given vector
    • Useful for approximating solutions and minimizing errors
  • Gram-Schmidt process is an algorithm for constructing an orthonormal basis from a linearly independent set of vectors
  • Cauchy-Schwarz inequality states that the absolute value of the inner product of two vectors is less than or equal to the product of their norms
    • u,vuv|\langle u, v \rangle| \leq \|u\| \|v\|

Inner Product Spaces

  • An inner product space is a vector space equipped with an inner product operation
  • Inner product is a function that takes two vectors and returns a scalar value
    • Denoted as u,v\langle u, v \rangle for vectors uu and vv
  • Inner product spaces allow us to define geometric concepts like angles, lengths, and orthogonality in abstract vector spaces
  • Examples of inner product spaces include:
    • Euclidean space Rn\mathbb{R}^n with the dot product
    • Space of continuous functions C[a,b]C[a, b] with the integral inner product f,g=abf(x)g(x)dx\langle f, g \rangle = \int_a^b f(x)g(x) dx
  • Inner product spaces have a rich structure and satisfy several important properties
    • Symmetry, linearity, and positive-definiteness
  • Many concepts from Euclidean geometry can be generalized to inner product spaces
    • Orthogonal projections, Gram-Schmidt process, and least-squares approximations

Properties of Inner Products

  • Symmetry: u,v=v,u\langle u, v \rangle = \langle v, u \rangle for all vectors uu and vv
  • Linearity in the first argument:
    • au,v=au,v\langle au, v \rangle = a\langle u, v \rangle for any scalar aa
    • u1+u2,v=u1,v+u2,v\langle u_1 + u_2, v \rangle = \langle u_1, v \rangle + \langle u_2, v \rangle for any vectors u1u_1, u2u_2, and vv
  • Positive-definiteness: v,v0\langle v, v \rangle \geq 0 for all vectors vv, with equality if and only if v=0v = 0
  • Cauchy-Schwarz inequality: u,vuv|\langle u, v \rangle| \leq \|u\| \|v\| for all vectors uu and vv
    • Equality holds if and only if uu and vv are linearly dependent
  • Norm induced by the inner product: v=v,v\|v\| = \sqrt{\langle v, v \rangle}
    • Satisfies the properties of a norm (non-negativity, homogeneity, and triangle inequality)
  • Parallelogram law: u+v2+uv2=2(u2+v2)\|u + v\|^2 + \|u - v\|^2 = 2(\|u\|^2 + \|v\|^2) for all vectors uu and vv

Orthogonality and Orthonormal Sets

  • Two vectors uu and vv are orthogonal if their inner product is zero: u,v=0\langle u, v \rangle = 0
    • Orthogonal vectors are perpendicular or at right angles to each other
  • An orthogonal set is a collection of non-zero vectors that are pairwise orthogonal
    • ui,uj=0\langle u_i, u_j \rangle = 0 for all iji \neq j
  • Orthonormal set is an orthogonal set where each vector has unit norm (length 1)
    • ui=1\|u_i\| = 1 for all vectors uiu_i in the set
  • Orthonormal sets are particularly useful as bases for inner product spaces
    • Coefficients of a vector with respect to an orthonormal basis are easily computed using inner products
  • Orthonormal bases simplify many computations and have desirable numerical properties
    • Minimize roundoff errors and provide a natural coordinate system
  • Examples of orthonormal sets include:
    • Standard basis vectors {e1,e2,,en}\{e_1, e_2, \ldots, e_n\} in Rn\mathbb{R}^n
    • Trigonometric functions {12π,1πcos(nx),1πsin(nx)}\{\frac{1}{\sqrt{2\pi}}, \frac{1}{\sqrt{\pi}}\cos(nx), \frac{1}{\sqrt{\pi}}\sin(nx)\} in L2[π,π]L^2[-\pi, \pi]

Gram-Schmidt Process

  • Gram-Schmidt process is an algorithm for constructing an orthonormal basis from a linearly independent set of vectors
  • Takes a linearly independent set {v1,v2,,vn}\{v_1, v_2, \ldots, v_n\} and produces an orthonormal set {u1,u2,,un}\{u_1, u_2, \ldots, u_n\}
  • The process works by iteratively orthogonalizing and normalizing the vectors
    1. Set u1=v1v1u_1 = \frac{v_1}{\|v_1\|}
    2. For i=2,,ni = 2, \ldots, n:
      • Compute the projection of viv_i onto the subspace spanned by {u1,,ui1}\{u_1, \ldots, u_{i-1}\}:
        • proji=j=1i1vi,ujujproj_i = \sum_{j=1}^{i-1} \langle v_i, u_j \rangle u_j
      • Subtract the projection from viv_i to obtain the orthogonal component:
        • ui=viprojiu_i' = v_i - proj_i
      • Normalize uiu_i' to obtain the orthonormal vector:
        • ui=uiuiu_i = \frac{u_i'}{\|u_i'\|}
  • The resulting set {u1,u2,,un}\{u_1, u_2, \ldots, u_n\} is an orthonormal basis for the subspace spanned by the original vectors
  • Gram-Schmidt process is widely used in numerical linear algebra and has applications in:
    • Least-squares approximations
    • QR factorization
    • Solving systems of linear equations

Orthogonal Projections

  • Orthogonal projection is the process of finding the closest point in a subspace to a given vector
  • Given a subspace WW and a vector vv, the orthogonal projection of vv onto WW is the unique vector projW(v)proj_W(v) in WW that minimizes the distance to vv
    • projW(v)=argminwWvwproj_W(v) = \arg\min_{w \in W} \|v - w\|
  • Orthogonal projection can be computed using an orthonormal basis {u1,,uk}\{u_1, \ldots, u_k\} for the subspace WW:
    • projW(v)=i=1kv,uiuiproj_W(v) = \sum_{i=1}^k \langle v, u_i \rangle u_i
  • Properties of orthogonal projections:
    • projW(v)proj_W(v) is the unique vector in WW such that vprojW(v)v - proj_W(v) is orthogonal to every vector in WW
    • projWproj_W is a linear transformation
    • projW(v)=vproj_W(v) = v if and only if vWv \in W
    • vprojW(v)vw\|v - proj_W(v)\| \leq \|v - w\| for all wWw \in W
  • Orthogonal projections have numerous applications, including:
    • Least-squares approximations and regression analysis
    • Signal and image processing (denoising, compression)
    • Solving systems of linear equations and optimization problems

Applications in Linear Algebra

  • Inner products and orthogonality have a wide range of applications in linear algebra and related fields
  • Least-squares approximations:
    • Finding the best approximation of a vector in a subspace
    • Minimizing the sum of squared errors between data points and a model
  • Orthogonal diagonalization of symmetric matrices:
    • Eigenvectors of a symmetric matrix form an orthonormal basis
    • Allows for efficient computation of matrix powers and exponentials
  • Principal component analysis (PCA):
    • Identifying the directions of maximum variance in a dataset
    • Useful for dimensionality reduction and data visualization
  • Quantum mechanics:
    • State vectors in a Hilbert space (an infinite-dimensional inner product space)
    • Observables represented by Hermitian operators with orthogonal eigenvectors
  • Fourier analysis and signal processing:
    • Representing functions as linear combinations of orthogonal basis functions (e.g., trigonometric functions, wavelets)
    • Analyzing and filtering signals in the frequency domain

Practice Problems and Examples

  1. Verify that the following functions define an inner product on the vector space of continuous functions C[0,1]C[0, 1]:
    • f,g=01f(x)g(x)dx\langle f, g \rangle = \int_0^1 f(x)g(x) dx
    • f,g=f(0)g(0)+01f(x)g(x)dx\langle f, g \rangle = f(0)g(0) + \int_0^1 f'(x)g'(x) dx
  2. Compute the orthogonal projection of the vector v=(1,2,3)v = (1, 2, 3) onto the subspace W=span{(1,1,1),(1,0,1)}W = \text{span}\{(1, 1, 1), (1, 0, -1)\} in R3\mathbb{R}^3.
  3. Apply the Gram-Schmidt process to the following set of vectors in R4\mathbb{R}^4:
    • v1=(1,0,0,0)v_1 = (1, 0, 0, 0), v2=(1,1,0,0)v_2 = (1, 1, 0, 0), v3=(1,1,1,0)v_3 = (1, 1, 1, 0), v4=(1,1,1,1)v_4 = (1, 1, 1, 1)
  4. Prove that if {u1,,un}\{u_1, \ldots, u_n\} is an orthonormal set in an inner product space VV, then for any vector vVv \in V:
    • v2=i=1nv,ui2+vi=1nv,uiui2\|v\|^2 = \sum_{i=1}^n |\langle v, u_i \rangle|^2 + \|v - \sum_{i=1}^n \langle v, u_i \rangle u_i\|^2
  5. Find the closest point in the plane x+y+z=1x + y + z = 1 to the point (2,3,4)(2, 3, 4) in R3\mathbb{R}^3.
  6. Determine whether the following sets of vectors are orthogonal, orthonormal, or neither:
    • {(1,1,0),(1,1,0),(0,0,1)}\{(1, 1, 0), (1, -1, 0), (0, 0, 1)\} in R3\mathbb{R}^3
    • {(1,0,1),(0,1,1),(1,1,0)}\{(1, 0, 1), (0, 1, 1), (-1, 1, 0)\} in R3\mathbb{R}^3
    • {sinx,cosx}\{\sin x, \cos x\} in L2[π,π]L^2[-\pi, \pi]
  7. Compute the Fourier coefficients of the function f(x)=x2f(x) = x^2 on the interval [π,π][-\pi, \pi] with respect to the orthonormal basis {12π,1πcos(nx),1πsin(nx)}\{\frac{1}{\sqrt{2\pi}}, \frac{1}{\sqrt{\pi}}\cos(nx), \frac{1}{\sqrt{\pi}}\sin(nx)\}.


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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.