**To answer the first question:**

This is the line element for a cylinder though the variable names might make more sense when the line element is written as, $ds^2 = dz^2 + r^2 d\phi^2$, where $r$ is a constant. In this context $z$ is the elevation on the cylinder, $r$ is the radius of the cylinder, $\phi$ is the angle which wraps around the cylinder.

Cylinders are flat because they can be cut and unfolded, making them into a rectangular sheet, without stretching the material of the cylinder. More formally there exists an isometric transformation from the cylinder to the plane. The identification of $\phi=0$ with $\phi=2\pi$ is a topological property of the cylinder which doesn't necessarily say anything about its curvature.

To be clear when I say that a transformation is isometric I meant that it preserves the relative distances of points as measured locally *within* the manifold. Distances measured through the embedding space are irrelevant.

Now suppose we wanted to map the plane to the sphere. We might start by turning the plane into a cylinder since we know we can do isometrically. To turn the cylinder into a sphere we would have to identify all the points on the rim at the top of the cylinder. The problem with this last identification is that it sends points that were formerly a finite distance apart to the same location meaning that the metric cannot have been preserved.

The above example isn't really a proof that there is not isometric mapping from a plane to a sphere, but I think it at least gives some insight into what is going on.

**To answer the second question:**

It looks like you are thinking of Identifying $\theta=0$ with $\theta=\pi$ and $\phi=0$ with $\phi=2\pi$ which would not form a sphere. Instead this would form a torus.

To form a sphere from $0 \leq \theta \leq \pi$ and $0\leq \phi \leq 2\pi$:

- For $ 0 < \theta < 2\pi $ identify $\phi=0$ with $\phi = 2\pi$.
- For $\theta = 0 $ identify all values of $\phi$ with a single point.
- For $\theta = \pi $ identify all values of $\phi$ with a single point.

An important thing to realize at this point is that we still don't have a proper sphere because we haven't defined a metric. As it stands our manifold could just be some deflated beach ball.

One line element which would be consistent with the boundary conditions is,

$$ds^2 = d\theta^2 + \theta(\pi-\theta) d\phi^2, $$

which is not the metric of a $2$-Sphere.