Ok, I got the escape velocity wrong, but you also missed:
wikipedia said:
The escape velocity can be thought of in terms of the speed an artillery shell or bullet fired from the surface would have to travel (ignoring the effects of drag) to leave orbit, but it is not the speed a rocket or other powered object would have to travel. An object under power could leave the Earth's gravity at any speed, assuming enough fuel.
Obviously blowing the moon is going to deliver a large enough force for it to accelerate, which means that many of the fragments are in principle powered objects. Escape velocity does not necessarily apply. If an object is already going at escape velocity then it doesn't matter, but even an object not going at escape velocity can still leave Earth provided its acceleration is large enough, and as I pointed out it doesn't have to be that large. In fact, if it is accelerating, it can quite easily reach the escape velocity before it stops accelerating. In particular, KE = W = (1/2)mv^2 = F*d*cos (theta), so force is still a pretty big factor in determining whether it escapes or not.
Not only that, but if you were to detonate inside the core, there has to be enough energy to actually blow out the outer portions of the moon, otherwise it will just simply be absorbed. Which requires that the velocity (and depending on the circumstances, its acceleration too) of the core fragments to be much larger than the fragments from the outer portions, since there is less energy by the time it even reaches the surface. So it doesn't really matter if the gravity near the center or core of the moon is lower than if you were to be on its surface. It doesn't change the energy requirements, which is dependent on their speed.
Another thing that I forgot to mention is Torque, centripetal acceleration and rotational velocity, because so far all of the calculations are assuming that the moon is stationary (The moon is orbiting and so has a centripetal acceleration, a rotational velocity and a rotational acceleration, and a velocity TANGENT to its orbit). For the fragments to actually fall to the Earth the torques have to cancel out, there has to be no rotational velocity, and its centripetal acceleration has to be lower than that of Earth's gravitational acceleration. A nuclear explosion releases energy in all directions, so for it to produce any torque whatsoever, the blast from the bombs would have to travel outward primarily in a single direction tangent to its orbit (I challenge you to do that!). So even if you do end of blowing up the moon most or even none of the fragments may actually fall to the Earth because most of it would still be orbiting. This is far more complicated than just relying on escape velocity, there are lots of conditions it has to meet.
So far, my points still stand. In fact, your calculations actually support my points now that I think about it.
No it isn't, it's the gravitational acceleration that determines its path, and the gravitational acceleration is independent of the object's mass. Two objects of totally different masses which start at the same position and initial velocity in a gravitational field will have exactly the same path.
And you missed my point completely. I said that acceleration determines the magnitude of the force, not whether or not it affected mass or its path. The same applies for gravity. And I had assumed that you knew what I meant, either its path is directly away from the Earth or at an angle to it, which would then lead to messy calculations involving force components.
Actually, if you really want a precise definition, F=dp/dt. Which is the change in momentum with respect to time. If the objects have a large enough change in momentum then they can leave Earth regardless of its direction...