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In the elementary proof of the slant surface area of a cone ##A=\pi r s##, where ##s## is the slant height, it is assumed that the net of a cone is a circular sector. In other words, if we cut the slant surface of a cone from its apex to its base along a straight line, the resulting surface can always be flatten out (onto a 2D plane without crumbling).
How do we prove that the resulting surface can always be flatten out?
This is no true for a hemisphere, for example.
How do we prove that the resulting surface can always be flatten out?
This is no true for a hemisphere, for example.