Ah, hell with it. I can't keep up this Haiku stuff. But here's the skinny:
1) special relativity can handle acceleration.
2) uniform gravity is just like acceleration.
One might come to the conclusion that special relativity should therefore be able to handle gravity. But it can't. Why? Well, consider two people on the opposite sides of the earth. Special relativity would need to treat both of them like they're accelerating away from each other, but they're clearly not. The problem is that the caveat of the gravitational field being uniform clearly doesn't hold here.
What general relativity does is use the concept that uniform gravity is just like acceleration in order to some up with a theory (really a GEOMETRY) to explain space-time.
People always obsess about this idea that gravity is just like acceleration, but I think the better way of looking at it is that any freefall is an inertial reference frame, that is, a free-falling object is NOT accelerating. In order for that to make sense, you need a curved space-time, so that "straight" (unaccelerating) trajectories through space-time looked curved to our naive Euclidean ideas of space.
So special relativity can handle acceleration. But only in a flat space-time. Once you throw in curvature from gravity, it becomes insufficient.