## Some integrable functions

Okay, we know what it means for a function to be integrable (in either of the equivalent Riemann or Darboux senses), but we don’t yet know any functions to actually be integrable. I won’t give the whole story now, but a just a large enough part to work with for the moment.

The major theorem here is that a continuous function on a closed interval is integrable. Notice from the Heine-Cantor theorem that is automatically uniformly continuous. That is, for any there is some so that for all and in with we have . Again, the important thing here is that we can choose our independently of the point , while continuity says might depend on .

So now we need to take our function and show that the upper and lower Darboux sums converge to the same value. Equivalently, we can show that their difference converges to zero. So given an we want to show that there is some partition so that the difference

is less than , and the same is true of any refinement of this partition.

We’ll choose our partition with every slice having constant width , so there are of them. By the uniform continuity of we can find a so that for any points and with we’ll have . Then in particular the difference will be less than , while and . Thus the difference in the Darboux sums will be less than , as we wanted.

What about refinements? Well, *any* refinement of a partition can only lower the upper Darboux sum and raise the lower one. This is because adding a point to a partition can’t raise the maximum in either of the new subintervals or lower the minimum, and in fact adding a point will usually lower the maximum and raise the minimum. So our partition has a small enough difference in the Darboux sums, and any refinement will make the difference even *smaller*, and thus we have the convergence we need.

Now, can we do better than continuous functions? Well, we can relax continuity at the endpoints a bit. If the function jumps to a different value at or than the limit seems to indicate, we can still get uniform continuity everywhere but that one point, and we’re still good. We still have problems with asymptotes where the function shoots off to infinity, like does at the left endpoint of .

What else? Well, we can allow a finite number of discontinuities, as long as none of them are asymptotes. If a discontinuity happens at , we can choose to be a partition point, and so on. Then a partition with these selected points is just the same as a partition on each of the continuous sections of the function in between the discontinuities, and we know that they’re all good.

Incidentally, we can use this same method of picking some of the partition points ahead of time to show another nice property of the integrals: we can break the integral in the middle of the interval and evaluate the two pieces separately, then add them together. That is, if then we have the equation

as long as both sides are integrable.