LightPhoton
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In all the sources I checked, except for one by Dwight E. Neuenschwander, Tensor Calculus for Physics: A Concise Guide, they only provide the definition of a tensor (or describe how it transforms). However, Neuenschwander attempts to motivate the definition of a second-rank tensor.
First, he defines the elements of the transformation matrix as
$$\Lambda_{\alpha i}=\langle \alpha\vert i \rangle= \frac{\partial x'^{\alpha}}{\partial x^i}$$
Then, Neuenschwander takes a general tensor, $\tilde I$, and represents it in the "Greek" basis as a transformation of tensor components in the "Latin" basis:
$$\langle \alpha\vert \tilde I\vert \beta \rangle=\langle \alpha\vert i\rangle\langle i\vert \tilde I\vert j\rangle\langle j\vert \beta \rangle \\ =\Lambda^{\alpha i}I^{ij}\Lambda^{j\beta}$$
At this point, Neuenschwander writes $$\Lambda^{j\beta}={\partial x'^{\beta}}/{\partial x^j}$$, but shouldn't it be $$\Lambda^{j\beta}={\partial x'^{j}}/{\partial x^\beta}?$$
First, he defines the elements of the transformation matrix as
$$\Lambda_{\alpha i}=\langle \alpha\vert i \rangle= \frac{\partial x'^{\alpha}}{\partial x^i}$$
Then, Neuenschwander takes a general tensor, $\tilde I$, and represents it in the "Greek" basis as a transformation of tensor components in the "Latin" basis:
$$\langle \alpha\vert \tilde I\vert \beta \rangle=\langle \alpha\vert i\rangle\langle i\vert \tilde I\vert j\rangle\langle j\vert \beta \rangle \\ =\Lambda^{\alpha i}I^{ij}\Lambda^{j\beta}$$
At this point, Neuenschwander writes $$\Lambda^{j\beta}={\partial x'^{\beta}}/{\partial x^j}$$, but shouldn't it be $$\Lambda^{j\beta}={\partial x'^{j}}/{\partial x^\beta}?$$