Nigel Wood
- 3
- 1
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.
Sorry about the Latex failure; I've no idea why I can't make it work on this site.
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