In quantum physics, if you are given the wave equation for a particle in an infinite square well, you may be asked to normalize the wave function. For example, start with the following wave equation:

The wave function is a sine wave, going to zero at *x* = 0 and *x* = *a*. You can see the first two wave functions plotted in the following figure.

Normalizing the wave function lets you solve for the unknown constant A. In a normalized function, the probability of finding the particle between

adds up to 1 when you integrate over the whole square well, *x* = 0 to *x* = *a*:

Substituting for

gives you the following:

Here’s what the integral in this equation equals:

So from the previous equation,

Solve for A:

Therefore, here’s the normalized wave equation with the value of A plugged in:

And that’s the normalized wave function for a particle in an infinite square well.