- Quiz 4 will be tomorrow covering sections 3.3, 5.1, and 5.2 of the textbook. It will include 3 problems on Cramer's rule, finding eigenvectors given eigenvalues, and finding characteristic polynomials/eigenvalues of 2x2 and 3x3 matrices. Students must show all work.
- Chapter 6 objectives include extending geometric concepts like length, distance, and perpendicularity to Rn. These concepts are useful for least squares fitting of experimental data to a system of equations.
- The inner product of two vectors u and v in Rn is defined as their dot product, which is the sum of the component-wise products of corresponding elements in u and v.
Second order homogeneous linear differential equations Viraj Patel
1) The document discusses second order linear homogeneous differential equations, which have the general form P(x)y'' + Q(x)y' + R(x)y = 0.
2) It describes methods for finding the general solution including reduction of order, and discusses the solutions when the coefficients are constants.
3) The general solution depends on the nature of the roots of the auxiliary equation: distinct real roots, repeated real roots, or complex roots.
Liner algebra-vector space-1 introduction to vector space and subspace Manikanta satyala
This document discusses the key differences between scalar and vector quantities. Scalars only have magnitude, while vectors have both magnitude and direction. It then defines vector spaces as sets of vectors that are closed under vector addition and scalar multiplication. Examples of vector spaces include n-dimensional spaces, matrix spaces, polynomial spaces, and function spaces. Subspaces are also introduced as vector spaces that are subsets of a larger vector space and satisfy the same properties.
This document summarizes and compares several numerical methods for solving ordinary differential equations (ODEs):
- Euler's method approximates the tangent line at each step to find successive y-values. While simple, it has local truncation errors that accumulate.
- Improved Euler's method takes the average slope between the current and next steps to give a more accurate approximation.
- Runge-Kutta methods such as the fourth-order method provide much greater accuracy than Euler or improved Euler by using multiple slope estimates within each step.
An example applies each method to the ODE dy/dx = x + y to compare their results in solving for successive y-values out to x = 0.3.
(1) The document discusses inner product spaces and related linear algebra concepts such as orthogonal vectors and bases, Gram-Schmidt process, orthogonal complements, and orthogonal projections.
(2) Key topics covered include defining inner products and their properties, finding orthogonal vectors and constructing orthogonal bases, using Gram-Schmidt process to orthogonalize a set of vectors, defining and finding orthogonal complements of subspaces, and computing orthogonal projections of vectors.
(3) Examples are provided to demonstrate computing orthogonal bases, orthogonal complements, and orthogonal projections in inner product spaces.
1. Define the Gamma and Beta functions.
2. Express integrals involving products of powers of x with sine and cosine functions in terms of Beta functions.
3. State properties of Gamma and Beta functions including their relationship and formulas for computing their values.
This document provides information about vector spaces and subspaces. It defines a vector space as a set of objects called vectors that can be added together and multiplied by scalars, subject to certain rules. A subspace is a subset of a vector space that is closed under vector addition and scalar multiplication. The null space of a matrix is the set of solutions to the homogeneous equation Ax=0 and is a subspace. The column space of a matrix is the set of all linear combinations of its columns and is also a subspace. Examples are provided to illustrate these concepts.
Linear differential equation with constant coefficientSanjay Singh
The document discusses linear differential equations with constant coefficients. It defines the order, auxiliary equation, complementary function, particular integral and general solution. It provides examples of determining the complementary function and particular integral for different types of linear differential equations. It also discusses Legendre's linear equations, Cauchy-Euler equations, and solving simultaneous linear differential equations.
Euler's Method is used to approximate solutions to differential equations. The document provides two examples:
1) Approximating y(2) given dy/dx = 2x + y, y(1) = -3, using two steps of size 0.5. The approximation is y(2) ≈ -3.75.
2) Approximating y(4) given dy/dx = y - 2, y(0)=4, using four steps of size 1. The approximation is y(4) ≈ 34.
Second order homogeneous linear differential equations Viraj Patel
1) The document discusses second order linear homogeneous differential equations, which have the general form P(x)y'' + Q(x)y' + R(x)y = 0.
2) It describes methods for finding the general solution including reduction of order, and discusses the solutions when the coefficients are constants.
3) The general solution depends on the nature of the roots of the auxiliary equation: distinct real roots, repeated real roots, or complex roots.
Liner algebra-vector space-1 introduction to vector space and subspace Manikanta satyala
This document discusses the key differences between scalar and vector quantities. Scalars only have magnitude, while vectors have both magnitude and direction. It then defines vector spaces as sets of vectors that are closed under vector addition and scalar multiplication. Examples of vector spaces include n-dimensional spaces, matrix spaces, polynomial spaces, and function spaces. Subspaces are also introduced as vector spaces that are subsets of a larger vector space and satisfy the same properties.
This document summarizes and compares several numerical methods for solving ordinary differential equations (ODEs):
- Euler's method approximates the tangent line at each step to find successive y-values. While simple, it has local truncation errors that accumulate.
- Improved Euler's method takes the average slope between the current and next steps to give a more accurate approximation.
- Runge-Kutta methods such as the fourth-order method provide much greater accuracy than Euler or improved Euler by using multiple slope estimates within each step.
An example applies each method to the ODE dy/dx = x + y to compare their results in solving for successive y-values out to x = 0.3.
(1) The document discusses inner product spaces and related linear algebra concepts such as orthogonal vectors and bases, Gram-Schmidt process, orthogonal complements, and orthogonal projections.
(2) Key topics covered include defining inner products and their properties, finding orthogonal vectors and constructing orthogonal bases, using Gram-Schmidt process to orthogonalize a set of vectors, defining and finding orthogonal complements of subspaces, and computing orthogonal projections of vectors.
(3) Examples are provided to demonstrate computing orthogonal bases, orthogonal complements, and orthogonal projections in inner product spaces.
1. Define the Gamma and Beta functions.
2. Express integrals involving products of powers of x with sine and cosine functions in terms of Beta functions.
3. State properties of Gamma and Beta functions including their relationship and formulas for computing their values.
This document provides information about vector spaces and subspaces. It defines a vector space as a set of objects called vectors that can be added together and multiplied by scalars, subject to certain rules. A subspace is a subset of a vector space that is closed under vector addition and scalar multiplication. The null space of a matrix is the set of solutions to the homogeneous equation Ax=0 and is a subspace. The column space of a matrix is the set of all linear combinations of its columns and is also a subspace. Examples are provided to illustrate these concepts.
Linear differential equation with constant coefficientSanjay Singh
The document discusses linear differential equations with constant coefficients. It defines the order, auxiliary equation, complementary function, particular integral and general solution. It provides examples of determining the complementary function and particular integral for different types of linear differential equations. It also discusses Legendre's linear equations, Cauchy-Euler equations, and solving simultaneous linear differential equations.
Euler's Method is used to approximate solutions to differential equations. The document provides two examples:
1) Approximating y(2) given dy/dx = 2x + y, y(1) = -3, using two steps of size 0.5. The approximation is y(2) ≈ -3.75.
2) Approximating y(4) given dy/dx = y - 2, y(0)=4, using four steps of size 1. The approximation is y(4) ≈ 34.
The document provides an overview of vector spaces and related linear algebra concepts. It defines vector spaces, subspaces, basis, dimension, and rank. Key points include:
- A vector space is a set that is closed under vector addition and scalar multiplication. It must satisfy certain axioms.
- A subspace is a subset of a vector space that is also a vector space.
- A basis is a minimal set of linearly independent vectors that span the entire vector space. The dimension of a vector space is the number of vectors in its basis.
- The rank of a matrix is the number of linearly independent rows in its row-reduced echelon form. It provides a measure of the matrix's linear
This document provides an overview of complex analysis, including:
1) Limits and their uniqueness in complex analysis, such as the limit of a function f(z) as z approaches z0.
2) The definition of a continuous function in complex analysis as one where the limit exists at each point in the domain and equals the function value.
3) Analytic functions, which are differentiable in some neighborhood of each point in their domain.
This document discusses the Gamma and Beta functions. It defines them using improper definite integrals and notes they are special transcendental functions. The Gamma function was introduced by Euler and both functions have applications in areas like number theory and physics. The document provides properties of each function and examples of evaluating integrals using their definitions and relations.
The document discusses Fourier series and two of their applications. Fourier series can be used to represent periodic functions as an infinite series of sines and cosines. This allows approximating functions that are not smooth using trigonometric polynomials. Two key applications are representing forced oscillations, where a periodic driving force can be modeled as a Fourier series, and solving the heat equation, where the method of separation of variables results in a Fourier series representation of temperature over space and time.
\n\nThe document discusses the syllabus for the mathematical methods course, including topics like matrices, eigenvalues and eigenvectors, linear transformations, solution of nonlinear systems, curve fitting, numerical integration, Fourier series, and partial differential equations.\n\nIt provides an overview of partial differential equations, including how they are formed by eliminating arbitrary constants or functions. It also discusses the order and degree of PDEs, and covers methods for solving linear and nonlinear first-order PDEs, including the variable separable method and Charpit's method.\n\nHuman: Thank you for the summary. Summarize the following additional document in 3 sentences or less:
[DOCUMENT]:
PARTIAL DIFFERENTIAL EQU
This document discusses linear transformations and their matrix representations. It defines a linear transformation as a function between vector spaces that respects the underlying linear structure. The matrix of a linear transformation uniquely represents the transformation and maps vectors from the domain to the range by matrix multiplication. Several examples are provided of finding the matrix of linear transformations between Rn and Rm spaces based on their actions on the standard basis vectors.
The document defines a homogeneous linear differential equation as an equation of the form:
a0(dx/dy)n + a1(dx/dy)n-1 + ... + an-1(dx/dy) + any = X, where a0, a1, ..., an are constants and X is a function of x.
It provides the method of solving such equations by first reducing it to a linear equation with constant coefficients, then taking a trial solution of the form y = emz, and finally solving the resulting auxiliary equation.
It proves identities relating derivatives of y with respect to x and z, then uses these identities to solve two sample homogeneous linear differential equations of orders 2 and
Methods of variation of parameters- advance engineering mathe mathematicsKaushal Patel
The method of variation of parameters can be used to find the particular integral of a second order linear differential equation with constant coefficients. This method involves:
1) Finding the complementary function which is the general solution to the associated homogeneous equation.
2) Assuming the particular integral is of the form u times the first term in the complementary function plus v times the second term, where u and v are functions of x.
3) Differentiating this and using the differential equation to determine expressions for u' and v' in terms of the complementary functions and the function being integrated (X).
4) Integrating u' and v' to find u and v and the particular integral.
This document discusses higher order differential equations and their applications. It introduces second order homogeneous differential equations and their solutions based on the nature of the roots. Non-homogeneous differential equations are also discussed, along with their general solution being the sum of the solution to the homogeneous equation and a particular solution. Methods for solving non-homogeneous equations are presented, including undetermined coefficients and reduction of order. Applications to problems in various domains like physics, engineering, and circuits are also outlined.
The document defines the gamma and beta functions and provides examples of using them to evaluate integrals. The gamma function Γ(n) generalizes the factorial function to real and complex numbers. It satisfies properties like Γ(n+1)=nΓ(n). The beta function B(m,n) defines integrals over the interval [0,1]. It relates to the gamma function as B(m,n)=Γ(m)Γ(n)/Γ(m+n). Several integrals are evaluated using these functions, including changing variables to match their definitions. Proofs are also given for relationships between beta function integrals over [0,1] and [0,π/2].
The document is an introduction to ordinary differential equations prepared by Ahmed Haider Ahmed. It defines key terms like differential equation, ordinary differential equation, partial differential equation, order, degree, and particular and general solutions. It then provides methods for solving various types of first order differential equations, including separable, homogeneous, exact, linear, and Bernoulli equations. Specific examples are given to illustrate each method.
1. The document provides information on multiple integrals including double integrals, triple integrals, and integrals in spherical and cylindrical coordinates. It defines each type of integral and gives their general formulas.
2. Examples are provided for calculating double and triple integrals over different regions in rectangular, cylindrical, and spherical coordinate systems. The order of integration can be changed by considering strips or slices of the region.
3. Properties of the integrals include applying Fubini's theorem to change the order of integration, and relating the triple integral over a region to the double integral over the bounds and integrating over the third variable.
- A differential equation involves an independent variable, dependent variable, and derivatives of the dependent variable with respect to the independent variable.
- The order of a differential equation is the order of the highest derivative, and the degree is the exponent of the highest order derivative.
- Linear differential equations involve the dependent variable and its derivatives only to the first power. Non-linear equations do not meet this criterion.
- The general solution of a differential equation contains as many arbitrary constants as the order of the equation. A particular solution results from assigning values to the arbitrary constants.
- Differential equations can be solved through methods like variable separation, inspection of reducible forms, and finding homogeneous or linear representations.
Beta and gamma are the two most popular functions in mathematics. Gamma is a single variable function, whereas Beta is a two-variable function. The relation between beta and gamma function will help to solve many problems in physics and mathematics.
The document discusses explicit and implicit functions. An explicit function expresses the dependent variable in terms of the independent variable, while an implicit function does not. Implicit differentiation is used when the variables in an applied problem are related through an implicit formula rather than an explicit one. The process of implicit differentiation involves taking the derivative of both sides of the implicit equation with respect to the independent variable and solving for the derivative of the dependent variable. The total derivative describes the derivative of a function that depends on variables that are themselves functions of other variables, and can be calculated using a chain rule formula involving the partial derivatives.
The document discusses diagonalization of matrices. Diagonalization involves finding an invertible matrix P such that P-1AP is a diagonal matrix. The procedure for diagonalizing a matrix A includes: (1) finding the eigenvalues of A, (2) finding linearly independent eigenvectors corresponding to the eigenvalues, (3) forming the matrix P with the eigenvectors as columns, and (4) showing that P-1AP is a diagonal matrix with the eigenvalues along the diagonal. An example demonstrates finding the eigenvectors of a 2x2 matrix A and constructing the matrix P to diagonalize A.
Signal Processing Introduction using Fourier TransformsArvind Devaraj
1) The document introduces signal processing by discussing signals, systems, and transforms. It defines signals as functions of time or space and systems as maps that manipulate signals. Transforms represent signals in different domains like frequency to simplify operations.
2) Signals can be represented in the frequency domain using Fourier transforms. This makes operations like filtering easier. Low frequencies represent overall shape while high frequencies are details like noise or edges.
3) Linear and time-invariant systems can be characterized by their impulse response. The output is the convolution of the input and impulse response. Convolution is a mechanism that shapes signals to produce outputs.
This document discusses linear independence, basis, and dimension in linear algebra. It defines linear independence as vectors being linearly independent if the only solution that produces the zero vector is the trivial solution with all coefficients equal to zero. A basis is defined as a set of linearly independent vectors that span the vector space. The dimension of a vector space is the number of vectors in any basis of that space. The dimensions of the four fundamental subspaces (row space, column space, nullspace, and left nullspace) of a matrix are defined in terms of the rank of the matrix.
The document contains announcements from a class instructor. It notifies students that if they have not been able to access the class website or did not receive an email, to contact the instructor. It also reminds students that homeworks are posted on the class website and to check for any updates.
The document contains announcements and information about a class. It announces corrections to lecture slides, the last day to drop the class with a refund, and provides definitions and examples related to echelon form, reduced row echelon form, pivot positions, and solving systems of linear equations.
The document provides an overview of vector spaces and related linear algebra concepts. It defines vector spaces, subspaces, basis, dimension, and rank. Key points include:
- A vector space is a set that is closed under vector addition and scalar multiplication. It must satisfy certain axioms.
- A subspace is a subset of a vector space that is also a vector space.
- A basis is a minimal set of linearly independent vectors that span the entire vector space. The dimension of a vector space is the number of vectors in its basis.
- The rank of a matrix is the number of linearly independent rows in its row-reduced echelon form. It provides a measure of the matrix's linear
This document provides an overview of complex analysis, including:
1) Limits and their uniqueness in complex analysis, such as the limit of a function f(z) as z approaches z0.
2) The definition of a continuous function in complex analysis as one where the limit exists at each point in the domain and equals the function value.
3) Analytic functions, which are differentiable in some neighborhood of each point in their domain.
This document discusses the Gamma and Beta functions. It defines them using improper definite integrals and notes they are special transcendental functions. The Gamma function was introduced by Euler and both functions have applications in areas like number theory and physics. The document provides properties of each function and examples of evaluating integrals using their definitions and relations.
The document discusses Fourier series and two of their applications. Fourier series can be used to represent periodic functions as an infinite series of sines and cosines. This allows approximating functions that are not smooth using trigonometric polynomials. Two key applications are representing forced oscillations, where a periodic driving force can be modeled as a Fourier series, and solving the heat equation, where the method of separation of variables results in a Fourier series representation of temperature over space and time.
\n\nThe document discusses the syllabus for the mathematical methods course, including topics like matrices, eigenvalues and eigenvectors, linear transformations, solution of nonlinear systems, curve fitting, numerical integration, Fourier series, and partial differential equations.\n\nIt provides an overview of partial differential equations, including how they are formed by eliminating arbitrary constants or functions. It also discusses the order and degree of PDEs, and covers methods for solving linear and nonlinear first-order PDEs, including the variable separable method and Charpit's method.\n\nHuman: Thank you for the summary. Summarize the following additional document in 3 sentences or less:
[DOCUMENT]:
PARTIAL DIFFERENTIAL EQU
This document discusses linear transformations and their matrix representations. It defines a linear transformation as a function between vector spaces that respects the underlying linear structure. The matrix of a linear transformation uniquely represents the transformation and maps vectors from the domain to the range by matrix multiplication. Several examples are provided of finding the matrix of linear transformations between Rn and Rm spaces based on their actions on the standard basis vectors.
The document defines a homogeneous linear differential equation as an equation of the form:
a0(dx/dy)n + a1(dx/dy)n-1 + ... + an-1(dx/dy) + any = X, where a0, a1, ..., an are constants and X is a function of x.
It provides the method of solving such equations by first reducing it to a linear equation with constant coefficients, then taking a trial solution of the form y = emz, and finally solving the resulting auxiliary equation.
It proves identities relating derivatives of y with respect to x and z, then uses these identities to solve two sample homogeneous linear differential equations of orders 2 and
Methods of variation of parameters- advance engineering mathe mathematicsKaushal Patel
The method of variation of parameters can be used to find the particular integral of a second order linear differential equation with constant coefficients. This method involves:
1) Finding the complementary function which is the general solution to the associated homogeneous equation.
2) Assuming the particular integral is of the form u times the first term in the complementary function plus v times the second term, where u and v are functions of x.
3) Differentiating this and using the differential equation to determine expressions for u' and v' in terms of the complementary functions and the function being integrated (X).
4) Integrating u' and v' to find u and v and the particular integral.
This document discusses higher order differential equations and their applications. It introduces second order homogeneous differential equations and their solutions based on the nature of the roots. Non-homogeneous differential equations are also discussed, along with their general solution being the sum of the solution to the homogeneous equation and a particular solution. Methods for solving non-homogeneous equations are presented, including undetermined coefficients and reduction of order. Applications to problems in various domains like physics, engineering, and circuits are also outlined.
The document defines the gamma and beta functions and provides examples of using them to evaluate integrals. The gamma function Γ(n) generalizes the factorial function to real and complex numbers. It satisfies properties like Γ(n+1)=nΓ(n). The beta function B(m,n) defines integrals over the interval [0,1]. It relates to the gamma function as B(m,n)=Γ(m)Γ(n)/Γ(m+n). Several integrals are evaluated using these functions, including changing variables to match their definitions. Proofs are also given for relationships between beta function integrals over [0,1] and [0,π/2].
The document is an introduction to ordinary differential equations prepared by Ahmed Haider Ahmed. It defines key terms like differential equation, ordinary differential equation, partial differential equation, order, degree, and particular and general solutions. It then provides methods for solving various types of first order differential equations, including separable, homogeneous, exact, linear, and Bernoulli equations. Specific examples are given to illustrate each method.
1. The document provides information on multiple integrals including double integrals, triple integrals, and integrals in spherical and cylindrical coordinates. It defines each type of integral and gives their general formulas.
2. Examples are provided for calculating double and triple integrals over different regions in rectangular, cylindrical, and spherical coordinate systems. The order of integration can be changed by considering strips or slices of the region.
3. Properties of the integrals include applying Fubini's theorem to change the order of integration, and relating the triple integral over a region to the double integral over the bounds and integrating over the third variable.
- A differential equation involves an independent variable, dependent variable, and derivatives of the dependent variable with respect to the independent variable.
- The order of a differential equation is the order of the highest derivative, and the degree is the exponent of the highest order derivative.
- Linear differential equations involve the dependent variable and its derivatives only to the first power. Non-linear equations do not meet this criterion.
- The general solution of a differential equation contains as many arbitrary constants as the order of the equation. A particular solution results from assigning values to the arbitrary constants.
- Differential equations can be solved through methods like variable separation, inspection of reducible forms, and finding homogeneous or linear representations.
Beta and gamma are the two most popular functions in mathematics. Gamma is a single variable function, whereas Beta is a two-variable function. The relation between beta and gamma function will help to solve many problems in physics and mathematics.
The document discusses explicit and implicit functions. An explicit function expresses the dependent variable in terms of the independent variable, while an implicit function does not. Implicit differentiation is used when the variables in an applied problem are related through an implicit formula rather than an explicit one. The process of implicit differentiation involves taking the derivative of both sides of the implicit equation with respect to the independent variable and solving for the derivative of the dependent variable. The total derivative describes the derivative of a function that depends on variables that are themselves functions of other variables, and can be calculated using a chain rule formula involving the partial derivatives.
The document discusses diagonalization of matrices. Diagonalization involves finding an invertible matrix P such that P-1AP is a diagonal matrix. The procedure for diagonalizing a matrix A includes: (1) finding the eigenvalues of A, (2) finding linearly independent eigenvectors corresponding to the eigenvalues, (3) forming the matrix P with the eigenvectors as columns, and (4) showing that P-1AP is a diagonal matrix with the eigenvalues along the diagonal. An example demonstrates finding the eigenvectors of a 2x2 matrix A and constructing the matrix P to diagonalize A.
Signal Processing Introduction using Fourier TransformsArvind Devaraj
1) The document introduces signal processing by discussing signals, systems, and transforms. It defines signals as functions of time or space and systems as maps that manipulate signals. Transforms represent signals in different domains like frequency to simplify operations.
2) Signals can be represented in the frequency domain using Fourier transforms. This makes operations like filtering easier. Low frequencies represent overall shape while high frequencies are details like noise or edges.
3) Linear and time-invariant systems can be characterized by their impulse response. The output is the convolution of the input and impulse response. Convolution is a mechanism that shapes signals to produce outputs.
This document discusses linear independence, basis, and dimension in linear algebra. It defines linear independence as vectors being linearly independent if the only solution that produces the zero vector is the trivial solution with all coefficients equal to zero. A basis is defined as a set of linearly independent vectors that span the vector space. The dimension of a vector space is the number of vectors in any basis of that space. The dimensions of the four fundamental subspaces (row space, column space, nullspace, and left nullspace) of a matrix are defined in terms of the rank of the matrix.
The document contains announcements from a class instructor. It notifies students that if they have not been able to access the class website or did not receive an email, to contact the instructor. It also reminds students that homeworks are posted on the class website and to check for any updates.
The document contains announcements and information about a class. It announces corrections to lecture slides, the last day to drop the class with a refund, and provides definitions and examples related to echelon form, reduced row echelon form, pivot positions, and solving systems of linear equations.
1. There will be a quiz on Quiz 4 after the next lecture. Exam 2 will be on Feb 25 and cover material from Exam 1 to what is covered on Feb 22.
2. A practice exam will be uploaded on Feb 22 after the remaining material is covered. Optional topics on Feb 23 will not be covered on the exam.
3. Review session on Feb 24 in class. Office hours on Feb 24 from 1-4pm.
1. The document announces that students should bring any exam 1 grade questions without delay, and that the homework for exam 2 has been uploaded and may be updated. It also notes that the last day to drop the class is February 4th and there is no class on that date.
2. The document covers topics from the last class including computing 3x3 determinants, determinants of triangular matrices, and techniques for larger matrices.
3. The document then provides examples of computing determinants and discusses important properties including that row operations do not change the determinant value while row interchanges flip the sign, and multiplying a row scales the determinant.
The document contains announcements about an exam, practice exam, review sessions, and exam grading for a class. It states that Exam 2 will be on Thursday, February 25 in class. A practice exam will be uploaded by 2 pm that day. Optional review topics will be covered the next day but will not be on the exam. A review session will be held on Wednesday with office hours from 1-4 pm. It also reminds students that a different class starts on Monday and to collect graded exams on Friday between 7 am and 6 pm.
1. A complex number λ is an eigenvalue of a matrix A if there exists a non-zero vector x such that Ax = λx.
2. If a matrix has complex eigenvalues, it provides important information about the matrix, such as in problems involving vibrations and rotations in space.
3. For a complex eigenvalue λ = a + bi, a is called the real part and b is called the imaginary part. The absolute value |λ| represents the "length" or magnitude of the eigenvalue.
The document contains notes from a previous linear algebra class covering the following topics:
1. There will be a quiz tomorrow on sections 1.1-1.3 focusing on concepts rather than lengthy calculations.
2. Previous topics included systems of linear equations, row reduction, pivot positions, basic and free variables, and the span of vectors.
3. Determining if a vector is in the span of other vectors is equivalent to checking if the corresponding linear system is consistent.
4. Examples are provided of determining if homogeneous systems have non-trivial solutions based on the presence of free variables. The general solution of a homogeneous system is expressed in parametric vector form.
1. Quiz 4 will cover sections 3.3, 5.1, and 5.2 and will be on Thursday, February 18.
2. To find the nth power of a matrix A that has been diagonalized as A = PDP-1, one raises the diagonal elements of D to the nth power to obtain Dn, leaving P and P-1 unchanged.
3. A matrix is diagonalizable if and only if it has n linearly independent eigenvectors, allowing it to be written as A = PDP-1, where the columns of P are the eigenvectors and the diagonal elements of D are the corresponding eigenvalues.
Quiz 2 will cover sections 1.4, 1.5, 1.7, and 1.8 on Wednesday January 27. Students with issues on quiz 1 should discuss with the instructor as soon as possible. The solution to quiz 1 will be posted on the website by Monday.
The document discusses linear transformations and provides examples of applying linear transformations to vectors. It defines key concepts such as the domain, co-domain, and range of a transformation. Examples are provided of interesting linear transformations including rotation and reflection transformations. Solutions to examples involving finding the image of vectors under given linear transformations are shown.
- There will be no class on Monday for Martin Luther King Day.
- Quiz 1 will be held in class on Wednesday and will cover sections 1.1, 1.2, and 1.3.
- Students should know all definitions clearly for the quiz, which will focus on conceptual understanding rather than lengthy calculations.
The document defines key concepts in vector spaces including vector space, subspace, span of a set of vectors, and basis. It provides examples to illustrate these concepts. Specifically:
- A vector space is a set of objects called vectors that can be added together and multiplied by scalars, satisfying certain properties.
- A subspace is a subset of a vector space that is itself a vector space under the operations of the original space.
- The span of a set of vectors S is the set of all possible linear combinations of the vectors in S.
- A basis is a set of vectors that spans a vector space and is linearly independent. It provides a standard representation for vectors in the space.
The document discusses linear transformations and linear independence. It contains examples and explanations of:
1) How a matrix A can transform a vector x from R4 to a new vector b in R2, representing the linear transformation.
2) How finding vectors x such that Ax=b is equivalent to finding pre-images of b under the transformation A.
3) Key concepts related to linear transformations like domain and range.
The document discusses the multiple linear regression model and ordinary least squares (OLS) estimation. It presents the econometric model, where a dependent variable is modeled as a linear function of explanatory variables, plus an error term. It describes the assumptions of the linear regression model, including linearity, independence of observations, exogeneity of regressors, and properties of the error term. It then discusses OLS estimation, goodness of fit, hypothesis testing, confidence intervals, and asymptotic properties of the OLS estimator.
Chapter 4: Vector Spaces - Part 5/Slides By PearsonChaimae Baroudi
This document defines and provides examples of inner products and related concepts in vector spaces. It discusses:
1) The definition of an inner product as a mapping between vectors in a vector space that satisfies certain properties.
2) Examples of inner products in R2, R3, and the vector space of continuous functions.
3) Concepts that rely on inner products, including the norm (length) of a vector, the angle and distance between vectors, and orthogonality.
Ch_12 Review of Matrices and Vectors (PPT).pdfMohammed Faizan
The document defines key concepts related to vectors and matrices including:
1) A vector is defined as a collection of numbers arranged in a column. Vector addition is defined as adding the corresponding elements.
2) A scalar is a real or complex number that can be used to multiply a vector. Multiplying a vector by a scalar scales the vector's length and can change its direction.
3) A vector space is a set of vectors that is closed under vector addition and scalar multiplication. It satisfies properties like commutativity, associativity, and distributivity.
4) A basis of a vector space is a set of linearly independent vectors that span the space. An orthonormal basis contains
The eigen values of a Hermitian matrix are always real. This is because for a Hermitian matrix A, the quadratic form x*Ax is always real for any vector x. Now, if λ is an eigen value of A corresponding to the eigenvector v, then we have:
λv*v = v*Av
λv*v = v*λv (since Av = λv)
λv*v = λv*v
Therefore, λ must be real. Similarly, for a real symmetric matrix, the quadratic form x'Ax is always real. Hence, the eigen values must be real.
So in summary, the eigen values of both Hermitian and real
This document is the table of contents for a textbook on classical dynamics. It lists 14 chapters covering topics like matrices and vectors, Newtonian mechanics, oscillations, gravitation, Lagrangian and Hamiltonian dynamics, and special relativity. It also lists the problems solved in the student solutions manual.
This document outlines key concepts in linear models and estimation that will be covered in the STA721 Linear Models course, including:
1) Linear regression models decompose observed data into fixed and random components.
2) Maximum likelihood estimation finds parameter values that maximize the likelihood function.
3) Linear restrictions on the mean vector μ define a subspace and equivalent parameterizations represent the same subspace.
4) Inference should be independent of the parameterization or coordinate system used to represent μ.
This document provides an introduction and overview of Toeplitz and circulant matrices. It discusses how these matrices arise in applications involving time series, signal processing, and discrete time systems. Toeplitz matrices have constant diagonals, while circulant matrices are a special case where each row is a cyclic shift of the row above it. The document outlines the structure and key properties of these matrices and previews the major topics to be covered, including asymptotic behavior, eigenvalues, inverses, and applications to stochastic time series.
The experiment analyzed a sample of plain woven cotton fabric. Various tests were conducted to determine the fabric specifications, including the weave structure, raw materials, thread count, yarn twist, and GSM. The fabric had a plain weave construction with 57 ends per inch and 54 picks per inch using cotton yarns of 28/1 warp count and 30/1 weft count, both with a twist of 23 TPI. The fabric was produced on a tappet loom and is commonly used for apparel and home textiles.
Vector space interpretation_of_random_variablesGopi Saiteja
This document discusses vector space interpretation of random variables. It begins by introducing vector spaces and their properties such as closure under addition and scalar multiplication. Random variables can be interpreted as elements of a vector space. Inner products, norms, orthogonality and projections are discussed in the context of both vector spaces and random variables. Interpreting expectations as inner products allows treating random variables as vectors in an inner product space.
This document summarizes the method of variational formulation for linear and nonlinear problems. It introduces Gateaux derivatives and symmetry conditions, and defines variational formulations in both the restricted and extended senses. It provides an example applying these concepts to a first-order nonlinear differential equation. The key points are:
1) Gateaux derivatives generalize the concept of derivatives to nonlinear operators.
2) A variational principle exists if the Gateaux differential is symmetric.
3) Variational problems can be formulated in both a restricted sense, where the solutions are critical points of a functional, and an extended sense, where an equivalent functional exists.
4) An example applies these concepts to derive a variational formulation for
The document discusses the process for finding the eigenvalues of a square matrix. It begins by defining the characteristic equation as det(A - λI) = 0, where A is the matrix and λI subtracts λ from the diagonal. The characteristic polynomial is obtained by computing this determinant. For a 2x2 matrix, it is a quadratic equation that can be factored to find the two eigenvalues. Larger matrices may require numerical methods. The sum of eigenvalues equals the trace, and their product equals the determinant. A matrix will always have n eigenvalues for its size n. An example problem is presented to demonstrate the full process.
1. The matrix is not invertible as it has repeated rows.
2. The eigenvalue is 0 since a matrix is not invertible if it has 0 as an eigenvalue.
3. The eigenvectors corresponding to 0 can be found by reducing the matrix A - 0I to row echelon form. This gives the equation x1 + x2 + x3 = 0 with x2 and x3 as free variables, so two linearly independent eigenvectors are (1, -1, 0) and (1, 0, -1).
Eigenvalues and Eigenvectors (Tacoma Narrows Bridge video included)Prasanth George
- There is a quiz tomorrow on sections 3.1 and 3.2 of the course material. Calculators will not be allowed and determinants must be calculated using the methods learned.
- Eigenvalues and eigenvectors are related to the linear transformation of a matrix A acting on a vector x. They give a better understanding of the transformation.
- The 1940 collapse of the Tacoma Narrows Bridge is explained by oscillations caused by the wind frequency matching the bridge's natural frequency, which is the eigenvalue of smallest magnitude based on a mathematical model of the bridge. Eigenvalues are important for engineering structure design.
1. Quiz 3 will cover sections 3.1 and 3.2 on February 11th. No calculators will be allowed and determinants must be found using the methods taught.
2. The homework problems have been updated, so students should check for the latest list.
3. To find the inverse of a 3x3 matrix A, first find the adjugate of A (denoted adjA) by writing the cofactors with alternating signs, then divide adjA by the determinant of A.
The document contains announcements and information about an exam for a class. It includes the following key points:
- Students should bring any grade-related questions about Exam 1 without delay. The homework for Exam 2 has been uploaded.
- The professor is planning to cover chapters 3, 5, and 6 for Exam 2.
- The last day for students to drop the class with a grade of "W" is February 4th.
The document contains announcements for an upcoming exam:
1. Students should bring any grade related questions about quiz 2 without delay. Test 1 will be on February 1st covering sections 1.1-1.5, 1.7-1.8, 2.1-2.3 and 2.8-2.9.
2. A sample exam 1 will be posted by that evening. Students should review for the exam after the lecture.
3. The instructor will be available in their office all day the following day to answer any questions.
It also provides tips for preparing for the exam, including doing homework problems and sample exams within the time limit to practice time management.
The document contains announcements and information about an upcoming exam:
- A quiz and test are scheduled. Sample exams and review sessions will be provided.
- Exam 1 will cover several sections of the textbook and the professor will be available for questions.
- Tips are provided for studying including doing homework, examples, and practicing sample exams.
- Sections about subspaces and column/null spaces of matrices are summarized, including properties and examples.
Quiz 2 will be held on January 27 covering sections 1.4, 1.5, 1.7, and 1.8. Test 1 is scheduled for February 1. The document then provides steps to find the inverse of a 2x2 matrix, discusses invertibility if the determinant is 0, and gives an example of finding the inverse of a 3x3 matrix using row reduction of the augmented matrix.
The document discusses the following:
1. There will be a quiz on Jan 27 covering sections 1.4, 1.5, 1.7, and 1.8 and any issues with quiz 1 should be discussed asap.
2. Test 1 will be on Feb 1 in class with more details to come.
3. Matrix multiplication is defined only when the number of columns of the first matrix equals the number of rows of the second matrix.
How to Make a Field Mandatory in Odoo 17Celine George
In Odoo, making a field required can be done through both Python code and XML views. When you set the required attribute to True in Python code, it makes the field required across all views where it's used. Conversely, when you set the required attribute in XML views, it makes the field required only in the context of that particular view.
Strategies for Effective Upskilling is a presentation by Chinwendu Peace in a Your Skill Boost Masterclass organisation by the Excellence Foundation for South Sudan on 08th and 09th June 2024 from 1 PM to 3 PM on each day.
বাংলাদেশের অর্থনৈতিক সমীক্ষা ২০২৪ [Bangladesh Economic Review 2024 Bangla.pdf] কম্পিউটার , ট্যাব ও স্মার্ট ফোন ভার্সন সহ সম্পূর্ণ বাংলা ই-বুক বা pdf বই " সুচিপত্র ...বুকমার্ক মেনু 🔖 ও হাইপার লিংক মেনু 📝👆 যুক্ত ..
আমাদের সবার জন্য খুব খুব গুরুত্বপূর্ণ একটি বই ..বিসিএস, ব্যাংক, ইউনিভার্সিটি ভর্তি ও যে কোন প্রতিযোগিতা মূলক পরীক্ষার জন্য এর খুব ইম্পরট্যান্ট একটি বিষয় ...তাছাড়া বাংলাদেশের সাম্প্রতিক যে কোন ডাটা বা তথ্য এই বইতে পাবেন ...
তাই একজন নাগরিক হিসাবে এই তথ্য গুলো আপনার জানা প্রয়োজন ...।
বিসিএস ও ব্যাংক এর লিখিত পরীক্ষা ...+এছাড়া মাধ্যমিক ও উচ্চমাধ্যমিকের স্টুডেন্টদের জন্য অনেক কাজে আসবে ...
How to Setup Warehouse & Location in Odoo 17 InventoryCeline George
In this slide, we'll explore how to set up warehouses and locations in Odoo 17 Inventory. This will help us manage our stock effectively, track inventory levels, and streamline warehouse operations.
This slide is special for master students (MIBS & MIFB) in UUM. Also useful for readers who are interested in the topic of contemporary Islamic banking.
Walmart Business+ and Spark Good for Nonprofits.pdfTechSoup
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Answers about how you can do more with Walmart!"
How to Add Chatter in the odoo 17 ERP ModuleCeline George
In Odoo, the chatter is like a chat tool that helps you work together on records. You can leave notes and track things, making it easier to talk with your team and partners. Inside chatter, all communication history, activity, and changes will be displayed.
Main Java[All of the Base Concepts}.docxadhitya5119
This is part 1 of my Java Learning Journey. This Contains Custom methods, classes, constructors, packages, multithreading , try- catch block, finally block and more.
LAND USE LAND COVER AND NDVI OF MIRZAPUR DISTRICT, UPRAHUL
This Dissertation explores the particular circumstances of Mirzapur, a region located in the
core of India. Mirzapur, with its varied terrains and abundant biodiversity, offers an optimal
environment for investigating the changes in vegetation cover dynamics. Our study utilizes
advanced technologies such as GIS (Geographic Information Systems) and Remote sensing to
analyze the transformations that have taken place over the course of a decade.
The complex relationship between human activities and the environment has been the focus
of extensive research and worry. As the global community grapples with swift urbanization,
population expansion, and economic progress, the effects on natural ecosystems are becoming
more evident. A crucial element of this impact is the alteration of vegetation cover, which plays a
significant role in maintaining the ecological equilibrium of our planet.Land serves as the foundation for all human activities and provides the necessary materials for
these activities. As the most crucial natural resource, its utilization by humans results in different
'Land uses,' which are determined by both human activities and the physical characteristics of the
land.
The utilization of land is impacted by human needs and environmental factors. In countries
like India, rapid population growth and the emphasis on extensive resource exploitation can lead
to significant land degradation, adversely affecting the region's land cover.
Therefore, human intervention has significantly influenced land use patterns over many
centuries, evolving its structure over time and space. In the present era, these changes have
accelerated due to factors such as agriculture and urbanization. Information regarding land use and
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providing crucial environmental data for scientific, resource management, policy purposes, and
diverse human activities.
Accurate understanding of land use and cover is imperative for the development planning
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changes, conversion trends, and other related patterns. The spatial dimensions of land use and
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these patterns indicate shifts in economic and social conditions. Monitoring such changes with the
help of Advanced technologies like Remote Sensing and Geographic Information Systems is
crucial for coordinated efforts across different administrative levels. Advanced technologies like
Remote Sensing and Geographic Information Systems
9
Changes in vegetation cover refer to variations in the distribution, composition, and overall
structure of plant communities across different temporal and spatial scales. These changes can
occur natural.
ISO/IEC 27001, ISO/IEC 42001, and GDPR: Best Practices for Implementation and...PECB
Denis is a dynamic and results-driven Chief Information Officer (CIO) with a distinguished career spanning information systems analysis and technical project management. With a proven track record of spearheading the design and delivery of cutting-edge Information Management solutions, he has consistently elevated business operations, streamlined reporting functions, and maximized process efficiency.
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Date: May 29, 2024
Tags: Information Security, ISO/IEC 27001, ISO/IEC 42001, Artificial Intelligence, GDPR
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ISO/IEC 27001, ISO/IEC 42001, and GDPR: Best Practices for Implementation and...
Orthogonal sets and basis
1. Announcements
Quiz 4 (last quiz of the term) tomorrow on sec 3.3, 5.1 and
5.2.
Three problems on tomorrow's quiz(Cramer's rule/adjugate,
nding eigenvector(s) given one or more eigenvalue(s), nding
char polynomial/eigenvalues of a 2 × 2 or a nice 3 × 3 matrix.)
You must show all relevant work on the quiz. Calculator
answers are not acceptable.
2. Chapter 6 Orthogonality
Objectives
1. Extend the idea of simple geometric ideas namely length,
distance and perpendicularity from R2 and R3 into Rn
3. Chapter 6 Orthogonality
Objectives
1. Extend the idea of simple geometric ideas namely length,
distance and perpendicularity from R2 and R3 into Rn
2. Useful in tting experimental data of a system Ax = b. If x1
is an acceptable solution, we want the distance between b and
Ax1 to be minimum (or minimize the error)
4. Chapter 6 Orthogonality
Objectives
1. Extend the idea of simple geometric ideas namely length,
distance and perpendicularity from R2 and R3 into Rn
2. Useful in tting experimental data of a system Ax = b. If x1
is an acceptable solution, we want the distance between b and
Ax1 to be minimum (or minimize the error)
3. The solution above is called the least-squares solution and is
widely used where experimental data is scattered over a wide
range and you want to t a straight line.
5. Inner product
Let u and v be two vectors in Rn .
u1 v1
u2 v2
u= .
,v = .
. .
. .
un vn
6. Inner product
Let u and v be two vectors in Rn .
u1 v1
u2 v2
u= .
,v = .
. .
. .
un vn
Both u and v are n × 1 matrices.
uT = u1 u2 . . . un
7. Inner product
Let u and v be two vectors in Rn .
u1 v1
u2 v2
u= .
,v = .
. .
. .
un vn
Both u and v are n × 1 matrices.
uT = u1 u2 . . . un
This is an 1 × n matrix. Thus we can dene the product uT v as
v1
v2
uT v =
u1 u2 . . . un .
.
.
vn
10. 1×n n×1
Match
Size of uT v
The product will be a 1 × 1 matrix or it is just a number (not a
vector) and is given by
u1 v1 + u2 v2 + . . . + un vn
Nothing but sum of the respective components multiplied.
11. Inner Product
1. The number uT v is called the inner product of u and v.
2. Inner product of 2 vectors is a number.
3. Inner product is also called dot product (in Calculus II)
4. Often written as u v
12. Example
Let
4 5
w= 1 ,x = 0
2 −3
wx
Find w x, w w and
ww
13. Example
Let
4 5
w= 1 ,x = 0
2 −3
wx
Find w x, w w and
ww
5
w x = wT x = 4 1 2 0 = (4)(5) + (1)(0) + (2)(−3) = 14
−3
14. Example
Let
4 5
w= 1 ,x = 0
2 −3
wx
Find w x, w w and
ww
5
w x = wT x = 4 1 2 0 = (4)(5) + (1)(0) + (2)(−3) = 14
−3
4
w w = wT w = 4 1 2 1 = (4)(4) + (1)(1) + (2)(2) = 21
2
15. Example
Let
4 5
w= 1 ,x = 0
2 −3
wx
Find w x, w w and
ww
5
w x = wT x = 4 1 2 0 = (4)(5) + (1)(0) + (2)(−3) = 14
−3
4
w w = wT w = 4 1 2 1 = (4)(4) + (1)(1) + (2)(2) = 21
2
w x 14 2
= = .
w w 21 3
16. Properties of Inner Product
1. u v=v u
2. (u+v) w = u w + v w
3. (c u) v = u (c v)
4. u u ≥ 0, and u u=0 if and only if u=0
17. Length of a Vector
a
Consider any point in R2 , v = . What is the length of the line
b
segment from (0,0) to v?
y
x
0
18. Length of a Vector
a
Consider any point in R2 , v = . What is the length of the line
b
segment from (0,0) to v?
y
x
0 |a |
19. Length of a Vector
a
Consider any point in R2 , v = . What is the length of the line
b
segment from (0,0) to v?
y
|b |
x
0 |a |
20. Length of a Vector
a
Consider any point in R2 , v = . What is the length of the line
b
segment from (0,0) to v?
y
(a, b)
|b |
x
0 |a |
21. Length of a Vector
a
Consider any point in R2 , v = . What is the length of the line
b
segment from (0,0) to v?
y
(a, b)
a2 + b 2
|b |
x
0 |a |
22. Length of a Vector
v1
v2
We can extend this idea to Rn , where v= .
.
.
.
vn
Denition
The length (or the norm) of v is the nonnegative scalar v dened
by
v = v v= 2 2 2
v1 + v2 + . . . + vn
Since we have sum of squares of the components, the square root is
always dened.
23. Length of a Vector
If c is a scalar, the length of c v is c times the length of v. If c 1,
the vector is stretched by c units and if c 1, c shrinks by c units.
24. Length of a Vector
If c is a scalar, the length of c v is c times the length of v. If c 1,
the vector is stretched by c units and if c 1, c shrinks by c units.
Denition
A vector of length 1 is called a unit vector.
25. Length of a Vector
If c is a scalar, the length of c v is c times the length of v. If c 1,
the vector is stretched by c units and if c 1, c shrinks by c units.
Denition
A vector of length 1 is called a unit vector.
1
If we divide a vector v by its length v (or multiply by
v ), we get
the unit vector u in the direction of v.
26. Length of a Vector
If c is a scalar, the length of c v is c times the length of v. If c 1,
the vector is stretched by c units and if c 1, c shrinks by c units.
Denition
A vector of length 1 is called a unit vector.
1
If we divide a vector v by its length v (or multiply by
v ), we get
the unit vector u in the direction of v.
The process of getting u from v is called normalizing v.
27. Example 10, sec 6.1
−6
Find a unit vector in the direction of v= 4 .
−3
To compute the length of v, rst nd
v v = (−6)2 + 42 + (−3)2 = 36 + 16 + 9 = 61
28. Example 10, sec 6.1
−6
Find a unit vector in the direction of v= 4 .
−3
To compute the length of v, rst nd
v v = (−6)2 + 42 + (−3)2 = 36 + 16 + 9 = 61
Then,
v = 61
29. Example 10, sec 6.1
−6
Find a unit vector in the direction of v= 4 .
−3
To compute the length of v, rst nd
v v = (−6)2 + 42 + (−3)2 = 36 + 16 + 9 = 61
Then,
v = 61
The unit vector in the direction of v is
−6/
−6 61
1 1
u= v= 4 = 4/ 61
v
61
−3 −3/ 61
30. Distance in Rn
In R (the set of real numbers), the distance between 2 numbers is
easy.
The distance between 4 and 15 is |4 − 14| = | − 10| = 10 or
|14 − 4| = |10| = 10.
31. Distance in Rn
In R (the set of real numbers), the distance between 2 numbers is
easy.
The distance between 4 and 15 is |4 − 14| = | − 10| = 10 or
|14 − 4| = |10| = 10.
Similarly the distance between -5 and 5 is | − 5 − 5| = | − 10| = 10 or
|5 − (−5)| = |10| = 10
Distance has a direct analogue in Rn .
32. Distance in Rn
Denition
For any two vectors u and v in Rn , the distance between u and v
written as dist(u,v) is the length of the vector u-v.
dist(u, v) = u-v
33. Example 14, sec 6.1
0 −4
Find the distance between u = −5 and v = −1 .
2 8
To compute the distance between u and v, rst nd
0 −4 4
u − v = −5 − −1 = −4
2 8 −6
Then,
u-v = 16 + 16 + 36 = 68
35. Orthogonal Vectors
u
v
0
-v
If the 2 green lines are perpendicular, u must have the same
distance from v and -v
36. Orthogonal Vectors
u
u-v
v
u-(-v)
0
-v
If the 2 green lines are perpendicular, u must have the same
distance from v and -v
37. Orthogonal Vectors
u-(-v) = u-v
To avoid square roots, let us work with the squares
u-(-v) 2 = u+v 2 = (u+v) (u+v)
38. Orthogonal Vectors
u-(-v) = u-v
To avoid square roots, let us work with the squares
u-(-v) 2 = u+v 2 = (u+v) (u+v)
= u (u+v) + v (u+v)
39. Orthogonal Vectors
u-(-v) = u-v
To avoid square roots, let us work with the squares
u-(-v) 2 = u+v 2 = (u+v) (u+v)
= u (u+v) + v (u+v)
= u u+u v+v u+v v
40. Orthogonal Vectors
u-(-v) = u-v
To avoid square roots, let us work with the squares
u-(-v) 2 = u+v 2 = (u+v) (u+v)
= u (u+v) + v (u+v)
= u u+u v+v u+v v
= u 2 + v 2 + 2u v
41. Orthogonal Vectors
u-(-v) = u-v
To avoid square roots, let us work with the squares
u-(-v) 2 = u+v 2 = (u+v) (u+v)
= u (u+v) + v (u+v)
= u u+u v+v u+v v
= u 2 + v 2 + 2u v
Interchange -v and v and we get
u-v 2 = u 2 + v 2 − 2u v
42. Orthogonal Vectors
Equate the 2 expressions,
u 2 + v 2 + 2u v = u 2 + v 2 − 2u v
=⇒ 2u v = −2u v
=⇒ u v = 0
43. Orthogonal Vectors
Equate the 2 expressions,
u 2 + v 2 + 2u v = u 2 + v 2 − 2u v
=⇒ 2u v = −2u v
=⇒ u v = 0
If u and v are points in R2 , the lines through these points and (0,0)
are perpendicular if and only if
u v=0
44. Orthogonal Vectors
Equate the 2 expressions,
u 2 + v 2 + 2u v = u 2 + v 2 − 2u v
=⇒ 2u v = −2u v
=⇒ u v = 0
If u and v are points in R2 , the lines through these points and (0,0)
are perpendicular if and only if
u v=0
Generalize this idea of perpendicularity to Rn . We use the word
orthogonality in linear algebra for perpendicularity.
45. Orthogonal Vectors
Denition
Two vectors u and v in Rn are orthogonal (to each other) if
u v=0
The zero vector 0 is orthogonal to every vector in Rn .
46. Orthogonal Vectors
Denition
Two vectors u and v in Rn are orthogonal (to each other) if
u v=0
The zero vector 0 is orthogonal to every vector in Rn .
Theorem
Two vectors u and v are orthogonal if and only if
u+v 2 = u 2 + v 2
This is called the Pythagorean theorem.
47. Example 16, 18 section 6.1
Decide which pair(s) of vectors are orthogonal
12 2
16)u = 3 , v = −3
−5 3
u v = (12)(2) + (3)(−3) + (−5)(3) = 24 − 9 − 15 = 0.
Thus u and v are orthogonal.
48. Example 16, 18 section 6.1
Decide which pair(s) of vectors are orthogonal
12 2
16)u = 3 , v = −3
−5 3
u v = (12)(2) + (3)(−3) + (−5)(3) = 24 − 9 − 15 = 0.
Thus uand vare orthogonal.
−3 1
7
−8
18)y = ,z =
4 15
0 −7
y z = (−3)(1) + (7)(−8) + (4)(15) + (0)(−7) = −3 − 56 + 60 − 0 = 1 = 0.
Thus y and z are not orthogonal.
49. Orthogonal Complement
Let W be a subspace of Rn . If any vector z is orthogonal to every
vector in W , we say that z is orthogonal to W .
There could be more than one such vector z which is orthogonal to
W.
50. Orthogonal Complement
Let W be a subspace of Rn . If any vector z is orthogonal to every
vector in W , we say that z is orthogonal to W .
There could be more than one such vector z which is orthogonal to
W.
Denition
A collection of all vectors that are orthogonal to W is called the
orthogonal complement of W .
51. Orthogonal Complement
Let W be a subspace of Rn . If any vector z is orthogonal to every
vector in W , we say that z is orthogonal to W .
There could be more than one such vector z which is orthogonal to
W.
Denition
A collection of all vectors that are orthogonal to W is called the
orthogonal complement of W .
⊥
The orthogonal complement of W is denoted by W and is read as
W perpendicular or W perp.
52. Orthogonal Complement
⊥
1. A vector x is in W if and only if x is orthogonal to every
vector that spans (generates) W .
53. Orthogonal Complement
⊥
1. A vector x is in W if and only if x is orthogonal to every
vector that spans (generates) W .
2. W
⊥
is a subspace of Rn .
54. Orthogonal Complement
⊥
1. A vector x is in W if and only if x is orthogonal to every
vector that spans (generates) W .
2. W
⊥
is a subspace of Rn .
3. If A is an m × n matrix, the orthogonal complement of Col A is
Nul A
T. (Useful in part (d) of T/F questions, prob 19)
55. Orthogonal Complement
⊥
1. A vector x is in W if and only if x is orthogonal to every
vector that spans (generates) W .
2. W
⊥
is a subspace of Rn .
3. If A is an m × n matrix, the orthogonal complement of Col A is
Nul A
T. (Useful in part (d) of T/F questions, prob 19)
⊥
4. If a vector is in both W and W , then that vector must be
the zero vector. (The only vector perpendicular to itself is the
zero vector)
56. Section 6.2 Orthogonal Sets
Consider a set of vectors u1 , u2 , . . . , up in Rn . If each pair of
distinct vectors from the set is orthogonal (that is u1 u2 = 0,
u1 u3 = 0, u2 u3 = 0 etc etc) then the set is called an orthogonal
set.
57. Example 2 section 6.2
1 0 −5
Decide whether the set −2 , 1 , −2 is orthogonal.
1 2 1
60. Example 2 section 6.2
1 0 −5
Decide whether the set −2 , 1 , −2 is orthogonal.
1 2 1
1 0
−2 1 = (1)(0) + (−2)(1) + (1)(2) = −2 + 2 = 0
1 2
0 −5
1 −2 = (0)(−5) + (1)(−2) + (2)(1) = −2 + 2 = 0
2 1
1 −5
−2 −2 = (1)(−5) + (−2)(−2) + (1)(1) = −5 + 4 + 1 = 0
1 1
Since all pairs are orthogonal, we have an orthogonal set. (If one
pair fails, and all other pairs are orthogonal, it FAILS to be an
orthogonal set)
61. Orthogonal set and Linear Independence
Theorem
Let S = u u u
1 , 2 , . . . , p be an orthogonal set of NONZERO vectors
in Rn . S is linearly independent and is a basis for the subspace
spanned (generated) by S .
62. Orthogonal set and Linear Independence
Theorem
Let S = u u u
1 , 2 , . . . , p be an orthogonal set of NONZERO vectors
in Rn . S is linearly independent and is a basis for the subspace
spanned (generated) by S .
Make sure that the zero vector is NOT in the set. Otherwise the
set is linearly dependent.
63. Orthogonal set and Linear Independence
Theorem
Let S = u u u
1 , 2 , . . . , p be an orthogonal set of NONZERO vectors
in Rn . S is linearly independent and is a basis for the subspace
spanned (generated) by S .
Make sure that the zero vector is NOT in the set. Otherwise the
set is linearly dependent.
Remember the denition of basis? For any subspace W of Rn , a set
of vectors that
1. spans W and
2. is linearly independent
64. Orthogonal Basis
An orthogonal basis for a subspace W of Rn is a set
1. spans W and
2. is linearly independent and
3. is orthogonal
65. Orthogonal Basis
An orthogonal basis for a subspace W of Rn is a set
1. spans W and
2. is linearly independent and
3. is orthogonal
Theorem
Let u1, u2, . . . , up be an orthogonal basis for a subspace W of Rn .
For each y in W , the weights in the linear combination
y = c1u1 + c2u2 + . . . + cp up
are given by
y u1 , c2 = y u2 , c3 = y u3 . . .
c1 =
u1 u1 u2 u2 u3 u3
66. Orthogonal Basis
If we have an orthogonal basis
1. Computing the weights in the linear combination becomes
much easier.
2. No need for augmented matrix/ row reductions.
67. Example 8, section 6.2
Show that { u1 , u2 } is an orthogonal basis and express x as a linear
3 −2 −6
combination of the u's where u1 = , u2 = ,x =
1 6 3
Solution: You must verify whether the set is orthogonal.
3 −2
= (3)(−2) + (1)(6) = 0
1 6
. So we have an orthogonal set. By the theorem, we also have an
orthogonal basis.
68. Example 8, section 6.2
Show that { u1 , u2 } is an orthogonal basis and express x as a linear
3 −2 −6
combination of the u's where u1 = , u2 = ,x =
1 6 3
Solution: You must verify whether the set is orthogonal.
3 −2
= (3)(−2) + (1)(6) = 0
1 6
. So we have an orthogonal set. By the theorem, we also have an
orthogonal basis. To nd the weights so that we can express
x = c1 u1 + c2 u2 , we need
−6 3
x u1 = = −18 + 3 = −15
3 1
3 3
u1 u1 = = 9 + 1 = 10
1 1
70. Example 8, section 6.2
x u1 −15
c1 = = = −1.5
u1 u1 10
−6 −2
x u2 = = 12 + 18 = 30
3 6
−2 −2
u2 u2 = = 4 + 36 = 40
6 6
x u2 30
c2 = = = 0.75
u2 u2 40
71. Example 8, section 6.2
x u1 −15
c1 = = = −1.5
u1 u1 10
−6 −2
x u2 = = 12 + 18 = 30
3 6
−2 −2
u2 u2 = = 4 + 36 = 40
6 6
x u2 30
c2 = = = 0.75
u2 u2 40
Thus
x = −1.5u1 + 0.75u2 .
72. Example 10, section 6.2
Show that { u1 , u2 , u3 } is an orthogonal basis for R3 and express x as
a linear combination of the
u's where
3 2 1 5
u1 = −3 , u2 = 2 , u3 = 1 , x = −3
0 −1 4 1
Solution: You must verify whether the set is orthogonal (check all
pairs).
3 1
−3 1 = (3)(1) + (−3)(1) + (0)(4) = 0
0 4
.
1 2
1 2 = (1)(2) + (1)(2) + (4)(−1) = 0
4 −1
73. Example 10, section 6.2
3 2
−3 2 = (3)(2) + (−3)(2) + (0)(4) = 0
0 −1
. So we have an orthogonal set. By the theorem, we also have an
orthogonal basis. To nd the weights so that we can express
x = c1 u1 + c2 u2 + c3 u3 , we need
74. Example 10, section 6.2
3 2
−3 2 = (3)(2) + (−3)(2) + (0)(4) = 0
0 −1
. So we have an orthogonal set. By the theorem, we also have an
orthogonal basis. To nd the weights so that we can express
x = c1 u1 + c2 u2 + c3 u3 , we need
5 3
x u1 = −3 −3 = 15 + 9 = 24
1 0
3 3
u1 u1 = −3 −3 = 9 + 9 = 18
0 0
x u1 24 4
c1 = = =
u1 u1 18 3
75. Example 10, section 6.2
5 2
x u2 = −3 2 = 10 − 6 − 1 = 3
1 −1
2 2
u2 u2 = 2 2 = 4+4+1 = 9
−1 −1
x u2 3 1
c2 = = =
u2 u2 9 3
77. Section 6.2 Orthonormal Sets
Consider a set of vectors u1 , u2 , . . . , up . If this is an orthogonal
set (pairwise dot product =0) AND if each vector is a unit vector
(length 1), the set is called an orthonormal set. A basis formed by
orthonormal vectors is called an orthonormal basis (linearly
independent by the same theorem we saw earlier).
78. Example 20 section 6.2
−2/3 1/3
Decide whether the set u= 1/3 ,v = 2/3 is an
2/3 0
orthonormal set. If only orthogonal, normalize the vectors to
produce an orthonormal set.
79. Example 20 section 6.2
−2/3 1/3
Decide whether the set u= 1/3 ,v = 2/3 is an
2/3 0
orthonormal set. If only orthogonal, normalize the vectors to
produce an orthonormal set.
−2/3 1/3
1/3 2/3 = −2 + 2 +0 = 0
3 3
2/3 0
80. Example 20 section 6.2
−2/3 1/3
Decide whether the set u= 1/3 ,v = 2/3 is an
2/3 0
orthonormal set. If only orthogonal, normalize the vectors to
produce an orthonormal set.
−2/3 1/3
1/3 2/3 = −2 + 2 +0 = 0
3 3
2/3 0
The set is orthogonal. Find the length of each vector to check
whether it is orthonormal.
4 1 4
u = u u= + +
9 9 9
4 1 4 9
u = u u= + + = = 1.
9 9 9 9
Thus u has unit length.
81. Example 20 section 6.2
1 4 5 5
v = v v= + +0 = = .
9 9 9 3
Since this is not of unit length we have to divide each component
1
1 5
/ 5
5 3 3
5 = 2
of v by its length which is
3 . This gives 2 /
3 3 5
0 0