Like Kummer said.
If you want to prove continuity at a point x_0, then your expression for \delta(\epsilon) may depend on x_0 too: \delta(\epsilon, x_0). And sometimes, like in the proof of the chain rule I think, it becomes necessary to specify that a number delta is the delta associated with epsilon, and x_0 and of the function f, and in that end, we shall write \delta(\epsilon, x_0, f).
Moreover, if a function is continuous on [a,b] say, then it means that given epsilon>0, there is a delta for every x in [a,b] and \delta(\epsilon, x) can be seen as a function sending x in [a,b] to a such proper delta. And if that \delta(\epsilon, x) function can be arranged to be constant over [a,b] (i.e. independant of x), this is when we say that f is uniformly continuous on [a,b].