Geodesics on a Hyperbolic Paraboloid Let $S \subset\mathbb{R}^3$ be a hyperbolic paraboloid and let $a,b \in S$.
I'm wondering how the Gauss-Bonnet Formula tells us that there is at most one geodesic $\gamma: [0,1] \rightarrow S$ such that $\gamma(0)=a$ and $\gamma(1)=b$.
\begin{equation}
\int_{S}KdA + \int_\gamma K_gds = 2 \pi
\end{equation}
Any help would be much appreciated!
 A: Choose a smooth normal vector field of unit length on the hyperbolic paraboloid and fix positive orientation on it, so that when you look from the tip of the vector down on the surface the positive orientation is counterclockwise. Assume you have two different geodesics $\gamma_1$ and $\gamma_2$ connecting points $a$ and  $b$. Then the two geodesics cut out a topological disc $S$, a geodesic bi-gon on the surface. Then, orient these geodesics as follow: $\gamma_1$ from $a$ to $b$ and $\gamma_2$ from $b$ to $a$. Let angle $\alpha > 0$ be the counterclockwise angle at $a$ from $\gamma_1$ to $\gamma_2$ and  Let angle $\beta > 0$ be the counterclockwise angle at $b$ from $\gamma_2$ to $\gamma_1$. Then clearly
$$\alpha + \beta > 0$$
The geodesic curvature of the closed piecewise geodesic loop $\gamma_1 \cup \gamma_2 = \partial \, S$ is zero everywhere except at the vertices $a$ and $b$ where it is $\pi - \alpha$ at $a$ and $\pi - \beta$ at $b$. Recall that the Gaussian curvature $K$ of the hyperbolic paraboloid is negative! Then by Gauss-Bonnet
$$\int_{S} \,K \, dA + \int_{\gamma_1 \cup \gamma_2} k_g = 2 \, \pi \, \chi(S) = 2 \pi$$  so 
$$\int_{S} \, K \, dA + 2 \pi - \alpha - \beta = 2 \pi$$ But then
$$0 > \int_S \, K \, dA  = \alpha + \beta$$ which is in a contradiction with the fact that $\alpha+\beta > 0$.
A: Hyperbolic paraboloid $S$ is given by $$ f(x,y)=(x,y,xy)$$
Consider $$ (x,0,0),\ (0,y,0)$$ which are geodesics in $\mathbb{R}$
Hence they are geodesics on $S$
In further $$f_x=(1,0,y),\ f_y=(0,1,x),\ E=1+y^2,\ G=1+x^2,\ F=xy
$$
\begin{align*} dA&=\sqrt{1+r^2}dxdy\\
\int_S K&= \int \frac{-1}{(1+r^2)^2} \sqrt{1+r^2} dxdy \\&=\int
\frac{-1}{(1+r^2)^\frac{3}{2}}\ rdrd\theta =2\pi
(1+r^2)^\frac{-1}{2}|_0^\infty=-2\pi\ \ast\end{align*}
Consider a geodesic triangle $\Delta$ : $(t,0,0),\ (0,t,0),\
(0,0,0),\ t>0$
Then $\int_\Delta K +\sum_i \theta_i=2\pi$ so that $$
\frac{\pi}{2}<\int_\Delta K+ \pi=\sum_i(\pi-\theta_i)$$
Here first inequality is followed since we have $\int_\Delta K>
\frac{1}{4}\int_S K$ by observing integrand in $\ast$ And last term
is sum of internal angles of $\Delta$ So we can not have a
contradiction
