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The journey to tensors begins with scalars and vectors.

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Chain Rule

Any differential divided by itself is one.

  •  \dfrac {dx}{dx} = 1
  •  \dfrac {dy}{dy} = 1
 \dfrac {du}{dz} = \dfrac {du}{dw} \dfrac {dw}{dx} \dfrac {dx}{dy}\dfrac {dy}{dz}

Can you see the cancellations for dw, dx and dy?

It is typical for a problem in Calculus I to make use of the following:

 \dfrac {df}{dx} = \dfrac {df}{du} \dfrac {du}{dx}

Appendix A

The Chain Rule carries (hides?) the idea of local flatness.

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