Yes, the situation makes more sense now.
You are picturing the induced charge on the inside surface of the conductor creating an oppositely induced charge on the outside surface near the location of the excess charge. The flaw is in assuming that that the charge "induced" on the outer surface must, in some manner, "reflect" the charge induced on the inner surface. This is not true, and it turns out that a uniform charge is induced all over the outer surface.
To get a better intuitive grasp of this, ask yourself what it means to say that the charge built up on the inner surface induces charge on the outer surface. Really, all that happens, is that free electrons redistribute themselves in response to say, a positive charge placed near the inside surface. In other words, free electrons from all parts of the conductor approach the inner surface, near the point where the positive charge lives. In doing so, they leave behind positively charged pockets where they came from. These pockets can also be treated as though they are mobile charges. So, these pockets, or holes, will want to get as far away from each other as possible, and they do this by:
(i) migrating to the outer surface, and
(ii) maintaining a uniform density there.
These holes, moreover, do not feel any effect from the electrons that are crowded near one spot on the inside, because, in the steady state, no electric field can propagate through the body of the conductor itself.