I have problem with following exercise

Consider the hypersurface $M$ parametrized by $z=x^2+y^2$.

Endow this with the Riemannian metric induced from the $\mathbb{R}^3$.

Compute the sectional curvature.

  • Bonnet-Myers theorem says that if the (Ricci) curvature is bounded from below by a positive constant then the manifold is compact. So, the given surface can't have curvature bounded from below by a positive constant. – mfl Nov 3 '14 at 10:15
  • Which parts do you have problem with? – user99914 Nov 3 '14 at 10:28
  • @John, How one can compute the sectional curvature of above? and i guess this calculation gives positive curvature, but this hypersurface is not compact. – phy_math Nov 3 '14 at 10:32
  • Do you know the metric of this surface? – user99914 Nov 3 '14 at 10:35
  • No.... Are you taking a course? – user99914 Nov 3 '14 at 10:40

I'd like to know my calculation process is done correctly.

Note $z=x^2+y^2$, in $\mathbb{R}^3$, by introducing spherical coordinate such that \begin{align} x= r\cos{\theta}, \quad y= r\sin{\theta} , \quad z=r^2 \end{align} we have \begin{align} x^2 +y^2 = r^2= z \end{align} and doing calculation with chain rule \begin{align} \partial_{r} = \cos(\theta)\partial_x + \sin(\theta) \partial_{y} +2r \partial_z\end{align} \begin{align} \partial_{\theta} = -r\sin(\theta) \partial_x + r\cos(\theta) \partial_y \end{align} Thus \begin{align} ds^2 = (1+4r^2)dr^2 + r^2d\theta^2 \end{align} and sectional curvature How can i use sectional curvature formula for this case?

I know

Note i used the formula for sectional curvature for geodesic polar coordinate $i.e$ \begin{align} ds^2 =dr^2 +f(r,\theta)^2 d\theta^2 \qquad K=-\frac{1}{f}\frac{\partial^2 f}{\partial r^2} \end{align}

  • I might be overlooking something, but it appears to me as though the surface that you have parametrized does not satisfy $z = x^2 + y^2$. Namely, I see that you have $x^2 + y^2 = \sin^{2}\theta_{1} \cos^{2}\theta_{2} + \sin^{2}\theta_{1} \sin^{2}\theta_{2} = \sin^{2}\theta_{1}$. By my calculations, this surface satisfies $x^2 + y^2 + z^1 = 1$ (i.e. is a sphere of radius 1). If you are going to introduce new coordinates to address the problem, you might consider spherical coordinates with $x = r\cos \theta$, $y = \r\sin \theta$ and $z = r^2$. – THW Nov 3 '14 at 18:12
  • 2
    It might be more instructive to set your surface up as a Monge surface with $(u, v)\mapsto (u, v, f(u, v))$ and derive the Gaussian curvature for a general Monge patch. – THW Nov 3 '14 at 18:20
  • @THW Thanks, I edited the process – phy_math Nov 4 '14 at 3:16
  • @THW, The informative for a general Monge patch helps me a lot. THanks – phy_math Nov 4 '14 at 3:35
  • I figure out what i did wrong in the above, and how to do this calculation correctly and obtain desired curvature. But still i am confused of considering Bonnet-Myers theorem. Maybe next week i will summarize my calculation and post it below. – phy_math Nov 4 '14 at 11:43
up vote 0 down vote accepted

This method was using Monge surface parametrization, which was introduced by @THW. in my former question.

Endowment of $\mathbb{R}^3$, we can do Gauss approach as follows. \begin{align} \mathbf{x}(r,\theta)=(f(r),r\cos(\theta), r\sin(\theta)) \end{align} where $f(r)=r^2=z$. \begin{align} &\mathbf{x}(r,\theta)=\left(f(r),r\cos(\theta), r\sin(\theta) \right) \quad \mathbf{x}_r = \left(f'(r), \cos(\theta), \sin(\theta) \right) \\ & \mathbf{x}_{rr} = \left( f''(r),0,0 \right) \quad \mathbf{x}_\theta = \left( 0,-r\sin(\theta), r\cos(\theta) \right) \\ &\mathbf{x}_{\theta\theta} = \left( 0,-r\cos(\theta), -r\sin(\theta) \right) \quad \mathbf{x}_{r\theta} = \left(0, -\sin(\theta), \cos(\theta)\right) \end{align} Here $'$ denote the $r$-derivative. Then \begin{align} I=ds^2 =(\mathbf{x}_r du + \mathbf{x}_\theta dv) \cdot(\mathbf{x}_r dr + \mathbf{x}_\theta d\theta) = Edr^2 + 2F drd\theta+ G d\theta^2 \end{align} with $E = 1 +(f')^2$, $F=0$, $G=r^2$. Note \begin{align} &\mathbf{x}_r \times \mathbf{x}_\theta = \left(r, -f'(r) r \cos(\theta), -f'(r) r \sin(\theta) \right) \\ &||\mathbf{x}_r \times \mathbf{x}_\theta|| = \sqrt{EG-F^2} = r\sqrt{1 + (f')^2} \\ & U=\frac{\mathbf{x}_r \times \mathbf{x}_\theta}{||\mathbf{x}_r \times \mathbf{x}_\theta||}= \frac{\left(1, -f' \cos(\theta), -f' \sin(\theta) \right)}{\sqrt{1 + (f')^2}} \end{align} and \begin{align} &e= \mathbf{x}_{rr} \cdot U=\frac{f''}{\sqrt{1 + (f')^2}}, \qquad f=\mathbf{x}_{r\theta}\cdot U=0 , \qquad g=\mathbf{x}_{\theta\theta} \cdot U=\frac{f'r}{\sqrt{1 + (f')^2}} \\ &\kappa_\mu = \frac{e}{E} =\frac{f''}{\sqrt{\left(1 +(f')^2 \right)^3}}, \quad \kappa_{\pi} = \frac{g}{G}=\frac{f'}{r\sqrt{1+(f')^2}} \end{align} Thus we obtain Gauss Curvature \begin{align} K = \kappa_\mu \kappa_\pi =\frac{f'f''}{r\left( 1 +(f')^2 \right)^2}\stackrel{f =r^2 }=\frac{4}{\left( 1 +4r^2 \right)^2} >0 \end{align}

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