Regrettable definition/notation

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Discussion Overview

The discussion revolves around the definitions of "Tensor Product" and "Dyadic Product" of vectors, highlighting apparent inconsistencies between mathematical and physical interpretations. Participants explore the implications of these definitions in the context of vector spaces and their duals.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants note that the mathematical definition of the tensor product as a bilinear function defined on V^* × V^* contrasts with the dyadic product defined as a linear operator on V.
  • One participant suggests that the bilinear function can be expressed as an operator, though questions arise regarding the definitions' domains.
  • Another participant proposes that the tensor product can be viewed as both a bilinear function and a linear function, indicating a potential overlap between the definitions.
  • There is a discussion about the action of the dyadic product on a vector, with a specific equation provided to illustrate this relationship.
  • Some participants express that while the definitions are not identical, they can be seen as natural and equivalent under certain conditions, particularly in finite-dimensional spaces with a scalar product.
  • Clarifications are made regarding the equivalence of various function types and the role of the internal product in the dyadic definition.

Areas of Agreement / Disagreement

Participants exhibit both agreement and disagreement, with some finding common ground on the equivalence of definitions under specific conditions, while others raise questions about the relationships between the definitions and their implications.

Contextual Notes

Participants acknowledge that the definitions depend on the existence of an internal product and the dimensionality of the vector spaces involved, which may limit the generalizability of their conclusions.

facenian
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hello, I would like to hear some comments about this situation. There seems to be two incompatible definitions concerning "Tensor Product" and "Dyadic product" of two vectors. The mathematical definition states tha [itex]a\otimes b[/itex] is a bilinear funtion defined on [itex]V^*\times V^*[/itex] with values in R while the dyadic product and also sometimes called tensor product written as ab and sometimes [itex]a\otimes b[/itex] is defined as a linear operator defined on V with values in V
I reached this conclution after looking up for the mathematical definition in "Tensor Analysis on Manifolds" by Bishop and for the definition used in physics in "Mechanics" by Symon, "Continuum Mechanics" by Chadwick,"Continuum Mechanics" by Spencer
 
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You'll probably find that the bilinear function can be written as an operator.
 
were the bilinear function defined on VxV or V*xV it would be possible but since it is denfined on V*xV* I don't know how to do it.
 
facenian said:
hello, I would like to hear some comments about this situation. There seems to be two incompatible definitions concerning "Tensor Product" and "Dyadic product" of two vectors. The mathematical definition states tha [itex]a\otimes b[/itex] is a bilinear funtion defined on [itex]V^*\times V^*[/itex] with values in R while the dyadic product and also sometimes called tensor product written as ab and sometimes [itex]a\otimes b[/itex] is defined as a linear operator defined on V with values in V
I reached this conclution after looking up for the mathematical definition in "Tensor Analysis on Manifolds" by Bishop and for the definition used in physics in "Mechanics" by Symon, "Continuum Mechanics" by Chadwick,"Continuum Mechanics" by Spencer

I can understand the first definition, but not the second. What I would think would be correct is this:

The tensor product of vectors [itex]a[/itex] and [itex]b[/itex] is a bilinear function of type [itex](V^*\times V^*) \rightarrow R[/itex], which is also a linear function of type [itex]V^*\rightarrow V[/itex]

(I'm using [itex]A \rightarrow B[/itex] to mean the type of functions that take objects of type [itex]A[/itex] and return objects of type [itex]B[/itex])
 
stevendaryl said:
I can understand the first definition, but not the second. What I would think would be correct is this:

The tensor product of vectors [itex]a[/itex] and [itex]b[/itex] is a bilinear function of type [itex](V^*\times V^*) \rightarrow R[/itex], which is also a linear function of type [itex]V^*\rightarrow V[/itex]

(I'm using [itex]A \rightarrow B[/itex] to mean the type of functions that take objects of type [itex]A[/itex] and return objects of type [itex]B[/itex])

The definition states the action of ab on a vector c through the equation:

[itex]a\otimes b (c)= (b.c)a[/itex] where b.c is the escalar product
 
facenian said:
The definition states the action of ab on a vector c through the equation:

[itex]a\otimes b (c)= (b.c)a[/itex] where b.c is the escalar product

Ah! Then I understand the two definitions. They aren't exactly the same, but they are both natural. If you have a scalar product, then there is NO difference between [itex]V[/itex] and [itex]V^*[/itex]. So all the following are equivalent:

  1. [itex](V^* \times V^*) \rightarrow R[/itex]
  2. [itex]V^* \rightarrow (V^* \rightarrow R)[/itex]
  3. [itex]V^* \rightarrow V^{**}[/itex]
  4. [itex]V^* \rightarrow V[/itex]
  5. [itex]V \rightarrow V[/itex]

1-3 are always equivalent. 4 is equivalent for finite-dimensional vector spaces, and 5 is equivalent for finite dimensional vectors spaces with a scalar product.
 
How is 3 equivalent to 1 or 2?
 
dauto said:
How is 3 equivalent to 1 or 2?

For any vector space [itex]V[/itex], the dual space [itex]V^*[/itex] is defined to be the linear functions of type [itex]V \rightarrow R[/itex].
 
Right!
 
  • #10
Simon Bridge said:
You'll probably find that the bilinear function can be written as an operator.
Yes, that's right. The piece of information I was not using is that the diad definition presupposes the existence of an internal product while the mathematical definition of tensor product does not. So taking into consideration the internal product we have a natural isomorphism between V* and V and finally both definitions coincide
 
  • #11
Well done: I knew you'd get there :)
 
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