Hmmm...seems to me we're all pretty much saying the same thing here.
According to my simulation, a typical curveball has a horzontal displacement of around a foot or so. Of course this is all dependant on the pitch speed, ball rotation speed, etc... I haven't gotten the assignment back yet, so I'm not ABSOLUTELY sure if my equations of motion and boundary conditions are right, but I think they are. The code to solve the differential equations is definitely correct, though. It's been tested in other situations. To be fair, I'm not worrying about the decay of rotational speed because it's pretty negligable over the time it takes the ball to travel from the pitcher to the catcher.
Turbo7 - I'm not a baseball player, and like I said above, maybe my math is simply incorrect, but the Magnus force seems to be roughly a third of the force of gravity. So in the case of a fastball, the rate of decent of the ball would be slowed, but the force would never be large enough for the vertical displacement to be negative (upwards) in relation to gravity. I think what's happening is that you're placing your catcher's mitt at a location where you'd expect the ball to be on a normal pitch, and finding that the ball doesn't drop as much as you expected it to - so you have to raise the mitt up a bit. My code shows a fastball of about 90mph to drop a little over a foot.