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2019, Springer eBooks
The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use.
This booklet contains an explanation about tensor calculus for students of physics and engineering with a basic knowledge of linear algebra. The focus lies mainly on acquiring an understanding of the principles and ideas underlying the concept of 'tensor'. We have not pursued mathematical strictness and pureness, but instead emphasise practical use (for a more mathematically pure resumé, please see the bibliography). Although tensors are applied in a very broad range of physics and mathematics, this booklet focuses on the application in special and general relativity.
This chapter is not meant as a replacement for a course in tensor analysis, but it will provide a working background to tensor notation and algebra.
2013
In general, a tensor is a multilinear transformation defined over an underlying finite dimensional vector space. In this brief introduction, tensor spaces of all integral orders will defined inductively. Initially the underlying vector space, V, will be assumed to be an inner product space in order to simplify the discussion. Subsequently, the presentation will be generalized to vector spaces without inner product. Usually, bold-face letters, a, will denote vectors in V and upper case letters, A, will denote tensors. The inner product on V will be denoted by a · b.
Tensors As mentioned in the introduction, all laws of continuum mechanics must be formulated in terms of quantities that are independent of coordinates. It is the purpose of this chapter to introduce such mathematical entities. We shall begin by introducing a shorthand notation-the indicial notation-in Part A of this chapter, which will be followed by the concept of tensors introduced as a linear transformation in Part B. The basic field operations needed for continuum formulations are presented in Part C and their representations in curvilinear coordinates in Part D. Part A The Indicia1 Notation 2A1 Summation Convention, Dummy Indices Consider the sum s = a p l + as2 + a3x3 +-* + a,&,, (2A1.1) We can write the above equation in a compact form by using the summation sign: n s = ajxi i = l (2A1.2) It is obvious that the following equations have exactly the same meaning as Eq. (2A1.2) n j=l s = 2 ajxj (2A1.3) n s = c a m x m m = l (2A1.4) etc. 3
Advances in Pattern Recognition, 2009
Tensors have been broadly used in mathematics and physics, since they are a generalization of scalars or vectors and allow to represent more complex properties. In this chapter we present an overview of some tensor applications, especially those focused on the image processing field. From a mathematical point of view, a lot of work has been developed about tensor calculus, which obviously is more complex than scalar or vectorial calculus. Moreover, tensors can represent the metric of a vector space, which is very useful in the field of differential geometry. In physics, tensors have been used to describe several magnitudes, such as the strain or stress of materials. In solid mechanics, tensors are used to define the generalized Hooke's law, where a fourth order tensor relates the strain and stress tensors. In fluid dynamics, the velocity gradient tensor provides information about the vorticity and the strain of the fluids. Also an electromagnetic tensor is defined, that simplifies the notation of the Maxwell equations. But tensors are not constrained to physics and mathematics. They have been used, for instance, in medical imaging, where we can highlight two applications: the diffusion tensor image, which represents how molecules diffuse inside the tissues and is broadly used for brain imaging; and the tensorial elastography, which computes the strain and vorticity tensor to analyze the tissues properties. Tensors have also been used in computer vision to provide information about the local structure or to define anisotropic image filters.
2006
The direct notation operates with scalars, vectors and tens ors as physical objects defined in the three dimensional space. A vector (first rank te sor)a is considered as a directed line segment rather than a triple of numbers (co ordinates). A second rank tensorA is any finite sum of ordered vector pairs A = a ⊗ b + . . . + c ⊗ d. The scalars, vectors and tensors are handled as invariant (inde pe nt from the choice of the coordinate system) objects. This is the reason for the us e of the direct notation in the modern literature of mechanics and rheology, e.g. [29 , 3 , 49, 123, 131, 199, 246, 313, 334] among others. The index notation deals with components or coordinates of v ectors and tensors. For a selected basis, e.g. gi, i = 1, 2, 3 one can write
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Tensor Network Contractions
This chapter is to introduce some basic definitions and concepts of TN. We will show that the TN can be used to represent quantum many-body states, where we explain MPS in 1D and PEPS in 2D systems, as well as the generalizations to thermal states and operators. The quantum entanglement properties of the TN states including the area law of entanglement entropy will also be discussed. Finally, we will present several special TNs that can be exactly contracted, and demonstrate the difficulty of contracting TNs in general cases. 2.1 Scalar, Vector, Matrix, and Tensor Generally speaking, a tensor is defined as a series of numbers labeled by N indexes, with N called the order of the tensor. 1 In this context, a scalar, which is one number and labeled by zero index, is a zeroth-order tensor. Many physical quantities are scalars, including energy, free energy, magnetization, and so on. Graphically, we use a dot to represent a scalar (Fig. 2.1). A D-component vector consists of D numbers labeled by one index, and thus is a first-order tensor. For example, one can write the state vector of a spin-1/2 in a chosen basis (say the eigenstates of the spin operatorŜ [z]) as |ψ = C 1 |0 + C 2 |1 = s=0,1 C s |s , (2.1) with the coefficients C a two-component vector. Here, we use |0 and |1 to represent spin up and down states. Graphically, we use a dot with one open bond to represent a vector (Fig. 2.1). 1 Note that in some references, N is called the tensor rank. Here, the word rank is used in another meaning, which will be explained later.
Tensors and their Applications, 2006
2001
Tensors are mathematical objects that generalize vectors and matrices. They describe geometrical quantities and they are used in various applied settings including mathematical physics. The indicial notation of tensors permits us to write an expression in a compact manner and to use simplifying mathematical operations. In a large number of problems in differential geometry and general relativity, the time consuming and straightforward algebraic manipulation is obviously very important. Thus, tensor computation came into existence and became necessary and desirable at the same time. Over the past 25 years, few algorithms have appeared for simplifying tensor expressions. Among the most important tensor computation systems, we can mention SHEEP, Macsyma !Tensor Package, MathTensor and GRTensorII. Meanwhile, graph theory, which had been lying almost dormant for hundreds of years since the time of Euler, started to explode by the turn of the 20th century. It has now grown into a major discipline in mathematics, which has branched off today in various directions such as coloring problems, Ramsey theory, factorization theory and optimization, with problems permeating into many scientific areas such as physics, chemistry, engineering, psychology, and of course computer science. Investigating some of the tensor computation packages will show that they have some deficiencies. Thus, rather than building a new system and adding more features to it, it was an objective in this thesis to express an efficient algorithms by removing most, if not all, restrictions compared to other packages, using graph theory. A summary of the implementation and the advantages of this system is also included. iii I am thankful to my supervisor, Professor Stephen Watt, who taught me everything I needed to know about tensor expressions, for accepting to supervise me, for his kindness and generous contributions of time and for his careful commentary of my thesis. Without him, this work would never been completed. Also, I would like to thank every person in the SCL lab for their helpful advice and useful comments on this thesis. Furthermore, I am sincerely grateful to my parents who kept supporting me regardless of the consequences and to my family, especially my wife, for their endless support and love. I shall never forget that.
American Journal of Physics, 2013
A guide on tensors is proposed for undergraduate students in physics or engineering that ties directly to vector calculus in orthonormal coordinate systems. We show that once orthonormality is relaxed, a dual basis, together with the contravariant and covariant components, naturally emerges. Manipulating these components requires some skill that can be acquired more easily and quickly once a new notation is adopted. This notation distinguishes multi-component quantities in different coordinate systems by a differentiating sign on the index labelling the component rather than on the label of the quantity itself. This tiny stratagem, together with simple rules openly stated at the beginning of this guide, allows an almost automatic, easy-to-pursue procedure for what is otherwise a cumbersome algebra. By the end of the paper, the reader will be skillful enough to tackle many applications involving tensors of any rank in any coordinate system, without indexmanipulation obstacles standing in the way. V
Universitext, 2005
Part I Basic Tensor Algebra Tensor Spaces 3 X Contents 3.5 Einstein's contraction of the tensor product 3.6 Matrix representation of tensors 3.6.1 First-order tensors 3.6.2 Second-order tensors 3.7 Exercises 4 Change-of-basis in Tensor Spaces 65 4.1 Introduction 65 4.2 Change of basis in a third-order tensor product space ....... 65 4.3 Matrix representation of a change-of-basis in tensor spaces ... 4.4 General criteria for tensor character 4.5 Extension to homogeneous tensors 4.6 Matrix operation rules for tensor expressions 74 4.6.1 Second-order tensors (matrices) 4.6.2 Third-order tensors 77 4.6.3 Fourth-order tensors 78 4.7 Change-of-basis invariant tensors: Isotropic tensors 4.8 Main isotropic tensors 4.8.1 The null tensor 4.8.2 Zero-order tensor (scalar invariant) 4.8.3 Kronecker's delta 4.9 Exercises
K24389 Illustrating the important aspects of tensor calculus, and highlighting its most practical features, Physical Components of Tensors presents an authoritative and complete explanation of tensor calculus that is based on transformations of bases of vector spaces rather than on transformations of coordinates. Written with graduate students, professors, and researchers in the areas of elasticity and shell theories in mind, this text focuses on the physical and nonholonomic components of tensors and applies them to the theories. It establishes a theory of physical and anholonomic components of tensors and applies the theory of dimensional analysis to tensors and (anholonomic) connections. This theory shows the relationship and compatibility among several existing definitions of physical components of tensors when referred to nonorthogonal coordinates. The book assumes a basic knowledge of linear algebra and elementary calculus, but revisits these subjects and introduces the mathematical backgrounds for the theory in the first three chapters. In addition, all field equations are also given in physical components as well. Comprised of five chapters, this noteworthy text: • Deals with the basic concepts of linear algebra, introducing the vector spaces and the further structures imposed on them by the notions of inner products, norms, and metrics • Focuses on the main algebraic operations for vectors and tensors and also on the notions of duality, tensor products, and component representation of tensors • Presents the classical tensor calculus that functions as the advanced prerequisite for the development of subsequent chapters • Provides the theory of physical and anholonomic components of tensors by associating them to the spaces of linear transformations and of tensor products and advances two applications of this theory Physical Components of Tensors contains a comprehensive account of tensor calculus , and is an essential reference for graduate students or engineers concerned with solid and structural mechanics.
Tensor Analysis, 2018
In Sect. 2.2.4 the Cauchy stress tensor T was defined. The stress tensor is the "original" tensor as the word tensor means stress. We shall use the definition of the stress tensor as an introduction to the general concept of tensors. We consider a body of continuous material and a material surface A in the body. At a place r a positive side of the surface is defined by a unit vector n as a normal pointing out from the surface. In a Cartesian coordinate system Ox with base vectors e k the normal vector n has the components: n k ; i.e. n ¼ n k e k : The contact force on the positive side of the surface is represented by the stress vector t with Cartesian components: t i ; i.e. t ¼ t i e i : The contact forces on positive coordinate surfaces through the place r are the stress vectors t k with Cartesian components T ik ; i.e. t k ¼ T ik e i : The components T ik are called the coordinate stresses. The Cauchy stress theorem by Eq. (2.2.27
2023
This booklet would like to whet your appetite to immerse yourself into the world of tensors with small bites of special tensors to take a closer look at tensor calculus. For the novice, tensor notations and operations are somehow clumsy and uncomfortable and accompanied by heavy calculations. Therefore here the focus is on praxis with selected examples - using Eigenmath as your computer algebraic companion to unburden calculation in this field.
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