For a regular parametric surface , set
The first fundamental form is the induced Riemannian metric
The second fundamental form, for this choice of unit normal vector, is
The Gaussian curvature is the product of the principal curvatures, equivalently the determinant of the shape operator:
Reversing the normal reverses the second fundamental form and both principal curvatures, while leaving unchanged.
Work on a regular patch with . Differentiating the surface of revolution gives
The arc-length condition gives , , . Also , so take
The second derivatives yield
Thus the first fundamental form and second fundamental form are
The opposite normal reverses the second displayed form. At a smooth pole the revolution coordinates degenerate, so curvature is understood by a regular local chart or by continuity.
Differentiating the arc-length identity gives . Multiply by and use to obtain
This derivation does not divide by , so it remains valid where . Inserting the first fundamental form and second fundamental form computed above gives the Gaussian curvature of a surface of revolution:
Choose and for . Adding the smooth poles at the endpoints gives the unit sphere. Its meridian is parametrized by arc length, and away from the poles, hence everywhere by continuity. Thus the unit sphere has constant Gaussian curvature one.
There is no compact smooth surface of revolution without boundary of constant Gaussian curvature minus one in this setting. On a compact such surface, the distance from the rotation axis attains a positive maximum. The maximum lies on a regular revolution patch, where the meridian arc length coordinate gives . Hence there, contradicting . Equivalently, constant negative curvature would require , excluding any positive radial maximum. Compact patches with boundary would not be excluded by this argument, but they are not closed surfaces.

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