The Rotational Surface with Zero Curvature
📂Geometry The Rotational Surface with Zero Curvature Theorem Let M M M be the unit speed curve of the rotational surface α \boldsymbol{\alpha} α and let the Gaussian curvature be K = 0 K=0 K = 0 . Then, M M M satisfies one of the following conditions.
It is a part of a cylinder. It is a part of a plane. It is a part of a cone. Moreover, these surfaces are locally isometric .
Proof Let the Gaussian curvature of the rotational surface be K = 0 K = 0 K = 0 . Since the curvature of the rotational surface is K = − r ′ ′ r K = -\dfrac{r^{\prime \prime}}{r} K = − r r ′′ , then r ′ ′ = 0 r^{\prime \prime} = 0 r ′′ = 0 . Therefore,
r ′ ′ ( s ) = 0 ⟹ r ′ ( s ) = a ⟹ r ( s ) = a s + b
r^{\prime \prime}(s) = 0 \implies r^{\prime}(s) = a \implies r(s) = as + b
r ′′ ( s ) = 0 ⟹ r ′ ( s ) = a ⟹ r ( s ) = a s + b
Since z ′ = ± 1 − ( r ′ ) 2 z^{\prime} = \pm\sqrt{1 - (r^{\prime})^{2}} z ′ = ± 1 − ( r ′ ) 2 ,
z ′ = ± 1 − ( r ′ ) 2 = ± 1 − a 2
z^{\prime} = \pm \sqrt{1 - (r^{\prime})^{2}} = \pm \sqrt{1 - a^{2}}
z ′ = ± 1 − ( r ′ ) 2 = ± 1 − a 2
⟹ z = ± 1 − a 2 s + d = c s + d
\implies z = \pm \sqrt{1-a^{2}}s + d = cs + d
⟹ z = ± 1 − a 2 s + d = cs + d
Thus, the curve α = ( r , z ) \boldsymbol{\alpha} = (r, z) α = ( r , z ) is as follows.
α ( s ) = ( r ( s ) , z ( s ) ) = ( a s + b , c s + d ) , a , b , c , d ∈ R
\boldsymbol{\alpha}(s) =\big(r(s), z(s)) = (as + b, cs + d),\quad a,b,c,d \in \mathbb{R}
α ( s ) = ( r ( s ) , z ( s )) = ( a s + b , cs + d ) , a , b , c , d ∈ R
If a = 0 a=0 a = 0 , then α ( s ) = ( b , c s + d ) \alpha (s) = (b, cs + d) α ( s ) = ( b , cs + d ) and the resulting rotational surface is part of a cylinder.
If c = 0 c=0 c = 0 , then α ( s ) = ( a s + b , d ) \alpha (s) = (as + b, d) α ( s ) = ( a s + b , d ) is a plane, and the resulting rotational surface is part of a plane.
If a ≠ 0 , c ≠ 0 a\ne 0, c\ne 0 a = 0 , c = 0 , then α ( s ) = ( a s + b , c s + d ) \alpha (s) = (as + b, cs + d) α ( s ) = ( a s + b , cs + d ) and this line is parallel to neither the r r r axis nor the z z z axis. The resulting rotational surface is part of a cone.
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