Is the Cauchy stress tensor really a tensor?

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    Cauchy Stress Tensor
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SUMMARY

The discussion centers on the Cauchy stress tensor and its classification as a tensor. The Cauchy stress tensor, denoted as ##\boldmath {\sigma}##, is defined by the equation ##\textbf{T}_e=\textbf{\sigma}~\textbf{e}##, where it transforms a unit normal vector ##\mathbf e## into a traction vector ##\textbf T##. Participants clarify that while the Cauchy stress tensor can take two vectors to produce a scalar, it can also take one vector and output another vector, thus adhering to the broader definition of tensors as multilinear maps. The discussion highlights the importance of understanding the nature of second-order tensors in the context of physics.

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Philip Wood
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I've just started learning about tensors from Jeevanjee's highly praised 'An Introduction to Tensors and Group Theory for Physicists'. He defines a tensor as a function, linear in each of its arguments, that takes some vectors (maybe only 2) and produces a number. [The components of the tensor are the values of this number when base vectors are the arguments.] The Cauchy stress tensor, ##\boldmath {\sigma}##, is, I read, defined by ##\textbf{T}_e=\textbf{\sigma}~\textbf{e}## in which the right hand side can be written as a multiplication a column vector of the components of the unit vector ##\mathbf e## normal to a surface by a matrix of components representing ##\textbf{\sigma}##. ##\textbf T## is another vector, the traction vector. So we seem to be inputting one vector and outputting another. This doesn't seem to fit Jeevanjee's definition of a tensor. Can someone explain?

Sorry about the Latex failure; I've no idea why I can't make it work on this site.
 
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Nigel Wood said:
I've just started learning about tensors from Jeevanjee's highly praised 'An Introduction to Tensors and Group Theory for Physicists'. He defines a tensor as a function, linear in each of its arguments, that takes some vectors (maybe only 2) and produces a number. [The components of the tensor are the values of this number when base vectors are the arguments.] The Cauchy stress tensor, ##\textbf \sigma##, is, I read, defined by ##\textbf{T}_e=\textbf{\sigma}~\textbf{e}## in which the right hand side can be written as a multiplication a column vector of the components of the unit vector ##\mathbf e## normal to a surface by a matrix of components representing ##\textbf{\sigma}##. ##\textbf T## is another vector, the traction vector. So we seem to be inputting one vector and outputting another. This doesn't seem to fit Jeevanjee's definition of a tensor. Can someone explain?
A rank-2 tensor like ##\sigma_{ij}## can indeed "take" two vectors and make a number (i.e., a scalar), but it can also "take" just one vector and turn it into another vector.
 
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Many thanks, renormalize. So Jeevanjee's being too restrictive? No wonder he doesn't use the Cauchy stress tensor as an example.
 
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Nigel Wood said:
Many thanks, renormalize. So Jeevanjee's being too restrictive? No wonder he doesn't use the Cauchy stress tensor as an example.
It's a long journey to learn about tensors. His definition is correct. As, @renormalize stated if you input a vector in one of the slots, you are left with a tensor that takes one less vector. This is similar to currying, or partial application if you are familiar with programming.
 
In a Mathematical sense, Tensors are generalizations of matrices for dimensions beyond 2, i.e., multilinear maps.
 
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My understanding is that a 2nd order tension (like the stress tensor) maps a given vector into another vector, the case of the stress tensor, the given vector is a unit normal vector to a surface, and the output vector is the traction vector on the surface.
 
Nigel Wood said:
Sorry about the Latex failure; I've no idea why I can't make it work on this site.
Looks like the \textbf command is treating its argument as literal text - i.e. not processing commands embedded in the text.

Using \mathbf doesn't seem to resolve this, - possibly because bold Greek letters aren't included in its font.

However \boldsymbol seems to work:
- a plain sigma looks like this: ##\sigma##.
- using \boldsymbol gives: ##\boldsymbol \sigma##

There may be other ways of course.
 
IIRC, one of the reasons is that it requires more than ##n ; n^2 ## entries to fully described in n-dimensions,
while a vector in n dimensions can be fully described with n components. The force, the normal, their interaction along each dimension.
 
Chestermiller said:
My understanding is that a 2nd order tension (like the stress tensor) maps a given vector into another vector, the case of the stress tensor, the given vector is a unit normal vector to a surface, and the output vector is the traction vector on the surface.
Many thanks. I'd better look into the concept of a second order tensor.
 

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