Fourier coefficients are essential components when working with Fourier series. They provide the weights for the different sine and cosine terms in the series. For a given function with period 2, we calculate the coefficients using integrals. The coefficients are divided into three types:
- The constant term, denoted as \(a_0\).
- The cosine coefficients, denoted as \(a_n\).
- The sine coefficients, denoted as \(b_n\).
The constant term \(a_0\) represents the average value of the function over one period. It's calculated by integrating the function over the period and dividing by the period length:
\[a_0 = \frac{1}{P} \int_{-L}^{L} f(x) \ dx\]
The cosine and sine coefficients, \(a_n\) and \(b_n\), are found similarly but involve multiplying the function by cosine or sine before integrating. This determines how much of each frequency component is present in the function:
\[a_n = \frac{2}{P} \int_{-L}^{L} f(x) \cos(\frac{n \pi x}{L}) \ dx\]
\[b_n = \frac{2}{P} \int_{-L}^{L} f(x) \sin(\frac{n \pi x}{L}) \ dx\]By calculating these coefficients, we capture the fundamental frequencies present in the function.