The Fourier series for a function \(f(x)\) defined over an interval, say \([-\pi, \pi]\), is given by:
$$ f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx)) $$
where the coefficients are calculated as:
$$ a_0 = \frac{1}{\pi} \int_{-\pi}^{\pi} f(x) dx $$
$$ a_n = \frac{1}{\pi} \int_{-\pi}^{\pi} f(x) \cos(nx) dx $$
$$ b_n = \frac{1}{\pi} \int_{-\pi}^{\pi} f(x) \sin(nx) dx $$
If the function \(f(x)\) is even, meaning \(f(-x) = f(x)\):
- The product \(f(x)\sin(nx)\) is an odd function (Even \(\times\) Odd = Odd).
The integral of an odd function over a symmetric interval like \([-\pi, \pi]\) is zero.
Therefore, \(b_n = 0\) for all \(n \ge 1\).
- The product \(f(x)\cos(nx)\) is an even function (Even \(\times\) Even = Even).
The integral of an even function over a symmetric interval is non-zero (unless f(x) itself leads to cancellation) and equals \( 2 \times \) the integral over half the interval.
Thus, \(a_n\) (for \(n \ge 1\)) can be non-zero.
- Similarly, \(a_0\) involves the integral of \(f(x)\) (an even function), which can be non-zero.
Therefore, the Fourier series for an even function contains only the constant term (\(a_0/2\)) and the cosine terms (\(a_n \cos(nx)\)).
It contains both \(a_0\) and \(a_n\) coefficients (while \(b_n\) are zero).
Option (3) is the best description.