Cylindrical polar co-ordinates

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The discussion focuses on using cylindrical polar coordinates to verify the divergence theorem with a specific vector field, A(r) = x(x-hat) + y(y-hat) + z^2(z-hat). The conversion between Cartesian and cylindrical coordinates is highlighted, particularly the relationships between the unit vectors rho-hat and phi-hat with respect to x and y. The user expresses confusion about the connection between these unit vectors and the Cartesian coordinates. A link to an overview of conversion formulas is provided for further clarification. Understanding these conversions is essential for applying the divergence theorem in cylindrical coordinates.
Nylex
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My notes have an example of verifying the divergence theorem using cylindrical polars.

There's a vector field, A(r) = x(x-hat) + y(y-hat) + z^2(z-hat) and my notes say:

"Note that rho-hat = cos phi(x-hat) + sin phi(y-hat) and phi-hat = -sin phi(x-hat) + cos phi(y-hat) and so

A(r) = rho(rho-hat) + z^2(z-hat)".

Why?? I can't see any obvious connection between phi-hat, rho-hat and x and y :confused:.
 
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Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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