In some applications, a function is defined only on the interval , and we need to find its Fourier series of period . We know how to find the Fourier series on a symmetric interval , so we need to extend somehow to the interval . After this we can extend to the entire real line by the periodicity condition .

There are two natural ways of extending . One is to obtain an *even* function
of period ,

The values of at 0 and integral multiples of do not affect the Fourier
series of . The Fourier series of will contain only cosine terms and is called the
**Fourier cosine series** of the original function .

The other canonical way of extending is to obtain an *odd* function
of period ,

The Fourier series of will contain only sine terms and is called the
**Fourier sine series** of the original function .

Figures 5 and 6 show the even and the odd extension respectively, for the function given on its half-period .

The choice of the extension depends on the concrete application in which we use Fourier series. For example, when the Fourier series is a possible solution to a differential equation, there is usually additional information available about the behaviour of the expected solution (e.g. boundary conditions). That information allows us to make the choice of the extension. However, the topic of applications of Fourier series is beyond the scope of this course, and you will always be told which extension to use.

**Example 7** The function
is given on its half-period. Find the even and the odd extensions, sketch their graphs.
Find the Fourier cosine and sine series of .

*Solution*:

We have to extend the function to the interval :

The graphs of the extensions are sketched in Figures 7 and 8, respectively.

For the Fourier cosine series we need to calculate and :

whence

For the Fourier sine series we need to calculate :

Then the Fourier **cosine** series is

and the Fourier **sine** series is

**Termwise Differentiation of Fourier Series**
In applications, if we consider Fourier series as a solution to a differential equation, we wish to substitute
by the series in the equation. In order to do so, we need to differentiate the series. In general, term-by-term differentiation of an infinite series is not always allowed. However, if the function is continuous and its derivative
is piecewise smooth, then the Fourier series of can be differentiated termwise, and