Lecture

Orthogonally Diagonalizable Matrices

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In course

MATH-111(pi): Linear algebra (flipped classroom)

L'objectif du cours est d'introduire les notions de base de l'algèbre linéaire et ses applications. Cette classe est donné sous forme inversée. ...

Description

This lecture covers the concept of orthogonally diagonalizable matrices, discussing logical conclusions and examples. It explains the conditions for a matrix to be orthogonally diagonalizable and the implications of this property. The lecture also delves into eigenvectors, bases, and the diagonalizability of matrix sums. Additionally, it explores the properties of clean vectors and the invertibility of matrices. The instructor presents various scenarios where matrices are or are not diagonalizable, providing insights into matrix operations and properties.

Instructors (2)

Simone Deparis

Expertise Simone Deparis is a professor at EPFL specializing in applied mathematics, numerical analysis, and the didactics of university-level mathematics. His research spans computational modeling for biomedical applications and innovations in mathematics education, with a focus on equity, self-efficacy, and assessment reform in large STEM cohorts. Mission Our group conducts research at the intersection of applied mathematics and learning sciences. In applied mathematics, we focus on modeling and simulatio

Donna Testerman

Teaching & PhD Past EPFL PhD Students Soumaïa Nadia Ghandour, Iulian Ion Simion, Mikaël Cavallin, Mikko Tapani Korhonen, Nathan Scheinmann, Ana Retegan, Jonathan Gruber

Official source

Ontological neighbourhood

Mathematics

Algebra: Linear algebra

Related concepts (32)

Invertible matrix

In linear algebra, an n-by-n square matrix A is called invertible (also nonsingular, nondegenerate or (rarely used) regular), if there exists an n-by-n square matrix B such that where In denotes the n-by-n identity matrix and the multiplication used is ordinary matrix multiplication. If this is the case, then the matrix B is uniquely determined by A, and is called the (multiplicative) inverse of A, denoted by A−1. Matrix inversion is the process of finding the matrix B that satisfies the prior equation for a given invertible matrix A.

Matrix (mathematics)

In mathematics, a matrix (plural matrices) is a rectangular array or table of numbers, symbols, or expressions, arranged in rows and columns, which is used to represent a mathematical object or a property of such an object. For example, is a matrix with two rows and three columns. This is often referred to as a "two by three matrix", a " matrix", or a matrix of dimension . Without further specifications, matrices represent linear maps, and allow explicit computations in linear algebra.

Matrix multiplication

In mathematics, particularly in linear algebra, matrix multiplication is a binary operation that produces a matrix from two matrices. For matrix multiplication, the number of columns in the first matrix must be equal to the number of rows in the second matrix. The resulting matrix, known as the matrix product, has the number of rows of the first and the number of columns of the second matrix. The product of matrices A and B is denoted as AB.

Diagonalizable matrix

In linear algebra, a square matrix is called diagonalizable or non-defective if it is similar to a diagonal matrix, i.e., if there exists an invertible matrix and a diagonal matrix such that , or equivalently . (Such , are not unique.) For a finite-dimensional vector space , a linear map is called diagonalizable if there exists an ordered basis of consisting of eigenvectors of .

Eigenvalues and eigenvectors

In linear algebra, an eigenvector (ˈaɪgənˌvɛktər) or characteristic vector of a linear transformation is a nonzero vector that changes at most by a constant factor when that linear transformation is applied to it. The corresponding eigenvalue, often represented by , is the multiplying factor. Geometrically, a transformation matrix rotates, stretches, or shears the vectors it acts upon. The eigenvectors for a linear transformation matrix are the set of vectors that are only stretched, with no rotation or shear.

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