Can Rank Two Tensors Be Formed Using Dot Products?

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In summary, Scott Smith is researching the foundations of rank two tensors. He is having trouble finding information or references on the subject, and asks for help. He is told that a rank two tensor can be written as T = T_{ij} \left( e_{i} \otimes e_{j} ) . Dot products can be formed using a basis that isn't orthonormal, and that ( u_i \otimes u_j ) \cdot ( u_k \otimes u_l ) = |u_i| |u_j| \cos \theta_{ij} |u_k| |u_l| \cos \theta_{kl}
  • #1
xGAME-OVERx
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Hi All,

I'm currently doing undergraduate research involving a lot of work with rank two Cartesian tensors, and I'm having trouble finding much information or good references on the foundations of such things.

It's my understanding that a rank two tensor can be written [tex] T = T_{ij} \left( e_{i} \otimes e_{j} ) [/tex]. Can dot products be formed something like [tex] ( e_i \otimes e_j ) \cdot ( e_k \otimes e_l ) [/tex] ?

I've seen some references that say that much as a vector has a (single) direction, a rank two tensors has two directions. Is this always true?

Thanks in Advance
Scott Smith
 
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  • #2
Yes, you can make dot products.

Two directions are ok for antisymmetric rank 2 tensors - but exactly speaking only "pure" ones. One day you will learn about "wedge product" - it is important.
 
  • #3
Thanks for the reply! I think I am aware of the wedge product, [tex] {\bf{a}} \wedge {{\bf{b}} = - {\bf{b}} \wedge {\bf{a}} [/tex], similar to the vector cross product?

So presumably [tex] ( e_i \otimes e_j ) \cdot ( e_k \otimes e_l ) = \delta_{ij} \delta_{kl} [/tex] for an orthonormal basis?

It is possible to use a basis that isn't orthonormal, say [tex] u_i [/tex], and define the dot product as [tex] ( u_i \otimes u_j ) \cdot ( u_k \otimes u_l ) = |u_i| |u_j| \cos \theta_{ij} |u_k| |u_l| \cos \theta_{kl} [/tex] ?
 
  • #4
I think you got mixed with the indices, it should be:


[tex] ( u_i \otimes u_j ) \cdot ( u_k \otimes u_l ) = |u_i| |u_k| \cos \theta_{ik} |u_j| |u_l| \cos \theta_{jl} [/tex]
As in [tex] ( u_i \otimes u_j ) \cdot ( u_k \otimes u_l ) = <u_i , u_k> <u_j, u_l>[/tex]
Or so I remeber it that way.
 
  • #5
Oops, sorry! Got the j and l indices backwards. Thanks!
 

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