Why Do Some Tensor Functions Appear Isotropic in Component Notation?

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SUMMARY

The discussion centers on the isotropy of tensor functions in component notation, specifically addressing the misconception that all tensor functions are isotropic. Andrea presents a mathematical framework involving Cartesian tensors, defining isotropic tensor functions as T = F(G) and demonstrating the transformation properties under rotation. The analysis reveals a critical error in assuming that the isotropy condition holds universally, as illustrated by the example of the anisotropic function H = g(T) = (T·(n⊗n))n⊗n, which does not satisfy isotropy for all orthogonal transformations Q.

PREREQUISITES
  • Understanding of Cartesian tensors and their properties
  • Familiarity with tensor notation and transformations
  • Knowledge of isotropic and anisotropic functions in continuum mechanics
  • Basic concepts of linear algebra, particularly orthogonal transformations
NEXT STEPS
  • Study the properties of isotropic tensor functions in detail
  • Explore the implications of anisotropic tensor functions in continuum mechanics
  • Learn about the mathematical framework of tensor transformations
  • Review Jaunzemis' Continuum Mechanics, particularly the sections on tensor functions
USEFUL FOR

This discussion is beneficial for mathematicians, physicists, and engineers specializing in continuum mechanics, particularly those working with tensor analysis and its applications in material science and structural analysis.

Andrea
Hello,

I consider only Cartesian tensors in the following. The definition of
isotropic tensor function I know is

1) T = F ( G )

such that, for any rotation ( ' = transpose),

2) O F( G ) O' = F( O G O' )

But, if I change to component notation, it seem to me that any tensor
function is isotropic, which cannot obviously be. Denoting the
components in the new basis with ^*, I have

3a) T_ij^* = O_ir T_rs (O_sj)'

3b) G_ij^* = O_ir G_rs (O_sj)'

since T and G are tensors. Then, by 1),

4a) T_rs = F_rs ( G_mn )

4b) T_rs^* = F_rs^* ( G_mn^* )

Then, substituting 3a) and 3b) into 4b), I get

5) O_ir T_rs (O_sj)' = F_rs^* ( O_mk G_kl (O_ln)' )

Finally, substituting 4a) into 5), I have

6) O_ir F_rs ( G_mn ) (O_sj)' = F_rs^* ( O_mk G_kl (O_ln)' )

that is,

O F( G ) O' = F (O G O' )

So any tensor function would be isotropic. Clearly that's false, but I
don't see where the error is. Can you help me find it? Thanks,

Andrea
 
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Here's an example of a tensor valued, anisotropic function

[tex]H = g(T) = (T\cdot{n\otimes{n}})n\otimes{n}[/tex]
where n is a fixed unit vector.

Then
[tex] g(QTQ^T) = (QTQ^T\cdot{n\otimes{n}})n\otimes{n} = (T \cdot (Q^Tn \otimes Q^Tn)) n\otimes{n}[/tex]
which is not the same as
[tex] Qg(T)Q^T = (T\cdot{n\otimes{n}})Qn\otimes{Qn} [/tex]
for general orthogonal Q, only if n is a proper vector of Q.
Im basically extrapolating from Jaunzemis' Continuum Mechanics book, pg 287.
 

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