The normal curvature, kn, is the curvature of the curve projected onto the plane containing the curve's tangent T and the surface normal u; the geodesic curvature, kg, is the curvature of the curve projected onto the surface's tangent plane
and normal curvature, "K_n"
The unit normal vector is given by (http://mathonline.wikidot.com/the-frenet-serret-formulas): "N(s)=\\frac{T'(s)}{||T'(s)||}" , where "T(s)=\\frac{\\vec{r}'(s)}{||\\vec{r}'(s)||}"
where "r(s)" is an arc-length parametrization of "\\vec{r}(t)"
"\\vec{r}(t)".
(a) We point out that one has an arc-length parametrization in this case. The length of the circle is "2\\pi" and it corresponds to the interval "[0,2\\pi)" for possible values of "t". Thus, t=s. We have:
"r'(t)=(-sin(t),cos(t),0)\\Rightarrow ||\\vec{r}'(t)||=1."
"T(t)=(-sin(t),cos(t),0)"; "T'(t)=(-cos(t),-sin(t),0)";
"N(t)=(-cos(t),sin(t),0)".
The geodesic curvature is (https://encyclopediaofmath.org/wiki/Geodesic_curvature):
"k_g=\\frac{(r',r'',n)}{|r'|^3}" , where "n" is a normal vector for the surface. The normal vector is:
"n=(2u,2v,-1)" (see https://mathworld.wolfram.com/NormalVector.html).
After substitution of the curve equation, we get that "n=(2cos\\,t,2sin\\,t,-1)" on the points of the curve. Thus,
"k_g=\\begin{vmatrix}\n -sin\\,t & cos\\,t &0 \\\\\n -cos\\,t & -sin\\,t &0\\\\\n2cos\\,t & 2sin\\,t &-1\n\\end{vmatrix}=-1"
The normal curvature is related to the second fundamental form, and an expression for it is
Where there is the surface on the paraboloid "\\sigma (u,v)=(u, v, u^2+v^2)" then
"L=\\sigma_{uu} \\cdot \\vec{N},\\ M=\\sigma_{uv} \\cdot \\vec{N}, L=\\sigma_{vv} \\cdot \\vec{N}," where "\\vec{N}" is the normal vector to the surface.
But on the paraboloid, "z=0". So, "\\sigma_{uu}=\\sigma_{uv}=\\sigma_{vv}=0" and also "L=M=N=0" thus "k_n=0"
Hence the solution for "K_g" and "K_n"
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