1, A.J.Mcconnell, applications of tensor  analysis, dover publications,Inc , NEW York
This presentation is the property of its rightful owner.
Sponsored Links
1 / 26

1, A.J.Mcconnell, applications of tensor analysis, dover publications,Inc , NEW York PowerPoint PPT Presentation


  • 87 Views
  • Uploaded on
  • Presentation posted in: General

1, A.J.Mcconnell, applications of tensor analysis, dover publications,Inc , NEW York 2, Garl E.pearson, handbook of applied mathematics, Van Nostrand Reinhold ; 2nd edition 3, I.s. sokolnikoff, tensor analysis, Walter de Gruyter ; 2Rev Ed edition

Download Presentation

1, A.J.Mcconnell, applications of tensor analysis, dover publications,Inc , NEW York

An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.


- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

Presentation Transcript


1 a j mcconnell applications of tensor analysis dover publications inc new york

1, A.J.Mcconnell, applications of tensor analysis, dover publications,Inc , NEW York

2, Garl E.pearson, handbook of applied mathematics, Van Nostrand Reinhold ; 2nd edition

3, I.s. sokolnikoff, tensor analysis, Walter de Gruyter ; 2Rev Ed edition

4. C.WREDE, introduction to vectors and tensor analysis, Dover Publications ; New Ed edition

5.WILHELM Flugge, tensor analysis and continuum mechanics , Springer ; 1 edition

6.Eutioquio C.young , vector and tensor analysis, CRC ; 2 edition

7. 黃克智,薛明德,陸明萬, 張量分析, 北京清華大學出版社


1 a j mcconnell applications of tensor analysis dover publications inc new york

Tensor analysis

1、Vector in Euclidean 3-D

2、Tensors in Euclidean 3-D

3、general curvilinear coordinates in Euclidean 3-D

4、tensorcalculus


1 vector in euclidean 3 d

1-1 Orthonormal base vector:

1、Vector in euclidean 3-D

Let (e1,e2,e3) be a right-handed

set of three mutually perpendicular

vector of unit magnitude


1 a j mcconnell applications of tensor analysis dover publications inc new york

ei(i = 1,2,3)may be used to define the kronecker delta δij and the permutation symbol eijk by means of the equations

and


1 a j mcconnell applications of tensor analysis dover publications inc new york

Ex1.

[prove]


1 a j mcconnell applications of tensor analysis dover publications inc new york

Thus δij = 1 for i=j ; e123 =e312=e231=1;e132=e321=e213=-1;

All other eijk = 0. in turn,a pair of eijk is related to a determinate of δij by

(1-1-1)

By setting r= i we recover the e – δrelation


1 a j mcconnell applications of tensor analysis dover publications inc new york

Rotated set of orthonormal base vector is introduced. the corresponding new components of F may be computed in terms of the old ones by writing

1-2 Cartesian component of vectors transformation rule

We have transformation rule

Here


1 a j mcconnell applications of tensor analysis dover publications inc new york

These direction cosines satisfy the useful relations

(1-2-1)

[prove]


1 a j mcconnell applications of tensor analysis dover publications inc new york

1-3 General base vectors:

vector components with respect to a triad of base vector need not be resticted to the use of orthonomal vector .let ε1, ε2 , ε3 be any three noncoplanar vector that play the roles of general base vectors


1 a j mcconnell applications of tensor analysis dover publications inc new york

(metric tensor)

and

(permutation tensor)

From (1-1-1) the general vector identity

can be established

(*)


1 a j mcconnell applications of tensor analysis dover publications inc new york

Note that the volume v of the parallelopiped having the base vectors as edges equals ; consequently the permutation tensor and the permutation symbols are related by

Denote by the determinate of the matrix having as its element

then, by (*), , so that


1 a j mcconnell applications of tensor analysis dover publications inc new york

1-4 General components of vectors ;transformation rules

convariant component

(free index)

contravariant component

(dummy index)

Summation notation:

the repeated index i, called “dummy index”, is to be summed

from 1 to n. This notation is due to Einstein.


1 a j mcconnell applications of tensor analysis dover publications inc new york

Figure. Convariant tensor and contravariant tensor in Euclidean 2-D

The two kinds of components can be related with the help of the metric tensor . Substituting into yields

[prove]


1 a j mcconnell applications of tensor analysis dover publications inc new york

Use to denote the (i , j)th element of the inverse of the matrix [g]

Where that the indices in the Kronecker delta have been placed in superscript and subscript position to conform to their placement on the left-hand side of the equation.

Proof.


1 a j mcconnell applications of tensor analysis dover publications inc new york

When general vector components enter , the summation convention invariably applies to summation over a repeated index that appears once as a superscript and once as a subscript

The metric tensor can introduce an auxiliary set of base vectors by means of means of the definition


1 a j mcconnell applications of tensor analysis dover publications inc new york

Consider , finally , the question of base vector , a direct calculation gives

for the transformed covariant components. We also find easily that


2 tensors in euclidean 3 d

2、Tensors in Euclidean 3-D

2-1 Dyads, dyadics, and second-order tensors

The mathematical object denote by AB, where A and B are given vectors, is called a dyad. The meaning of AB is simply that the operation

A sum of dyads, of the form

Is called a dyadic


1 a j mcconnell applications of tensor analysis dover publications inc new york

Any dyadic can be expressed in terms of an arbitrary set of general base vectors εi ;since

It follows that

T can always be written in the form

(2-1-1)

(contravariant components of the tensor).


1 a j mcconnell applications of tensor analysis dover publications inc new york

We re-emphasize the basic meaning of T by noting that ,for all vector V

By introduce the contravariant base vectors єi we can define other kinds of components of the tensor T. thus, substituting

Into (2-1-1), we get

Where are nine quantities


1 a j mcconnell applications of tensor analysis dover publications inc new york

are called the covariantcomponent of the tensor. Similarly ,we can define two, generally ,kinds of mixed components

That appear in the representation


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.2 Transformation rule

Suppose new base vectors are introduced; what are the new components of T? substitution

Into (2-1-1) gives

Is the desired transformation rule. Many different, but equivalent, relations are easily derived;for example


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.3 Cartesian components of second-order Tensors

Cartesian components


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.4 Tensors operations

Quotient laws


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.5 The metric Tensor

Substituting


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.6 Nth _ order Tensors

A third-order tensor, or triadic, is the sum of triads ,as follows:

It is easily established that any third-order tensor can written

As well as in the alternative form

N indices

N base vectros


1 a j mcconnell applications of tensor analysis dover publications inc new york

2.7 The permutation tensor

Choose a particular set of base vectors ,and define the third –order tensor

(2-4-1)

Since it follow that E has the same from as (2-4-1) with respect to all sets of base vector , so is indeed a tensor


  • Login