Applying definite integrals

For a discussion on the basic theory of integrals see: w:Riemann sum

Imagine an object that is free to move in one dimension — say, along the  axis. Like every physical object, it has a more or less fuzzy position (relative to whatever reference object we choose). For the purpose of describing its fuzzy position, quantum mechanics provides us with a probability density  This depends on actual measurement outcomes, and it allows us to calculate the probability of finding the particle in any given interval of the  axis, provided that an appropriate measurement is made.

We call a probability density because it represents a probability per unit length. The probability of finding in the interval between and  is given by the area  between the graph of the  axis, and the vertical lines at and  respectively. How do we calculate this area? The trick is to cover it with narrow rectangles of width

The area of the first rectangle from the left is the area of the second is and the area of the last is For the sum of these areas we have the shorthand notation

It is not hard to visualize that if we increase the number of rectangles and at the same time decrease the width of each rectangle, then the sum of the areas of all rectangles fitting under the graph of between and  gives us a better and better approximation to the area  and thus to the probability of finding in the interval between and  As tends toward 0 and tends toward infinity (), the above sum tends toward the integral

We sometimes call this a definite integral to emphasize that it's just a number. (As you can guess, there are also indefinite integrals, about which more later.) The uppercase delta has turned into a  indicating that is an infinitely small (or infinitesimal) width, and the summation symbol (the uppercase sigma) has turned into an elongated S indicating that we are adding infinitely many infinitesimal areas.

Don't let the term "infinitesimal" scare you. An infinitesimal quantity means nothing by itself. It is the combination of the integration symbol with the infinitesimal quantity that makes sense as a limit, in which grows above any number however large, (and hence the area of each rectangle) shrinks below any (positive) number however small, while the sum of the areas tends toward a well-defined, finite number.