Concept:
Any periodic function f(t) of period T = 2π has a Fourier series given by,
\(f\left( t \right) = {a_0} + {\rm{\Sigma }}{n = 1}^\infty ;{a_n}\cos nt + {\rm{\Sigma }}{n = 1}^\infty ;{b_n}\sin nt\)
where an , bn & ao are called coefficients
\({a_n} = \frac{2}{T}\mathop \smallint \limits_0^T f\left( t \right)\cos n{\omega _o}t;dt\) , \({b_n} = \frac{2}{T}\mathop \smallint \limits_0^T f\left( t \right)\sin n\omega t;dt\)
Explanation:
\(f\left( t \right) = \left{ {\begin{array}{*{20}{c}} {A\sin t,}&{0 \le t \le \pi }\ {0,}&{\pi < t < 2\pi } \end{array}} \right.\)
\({a_n} = \frac{2}{T}\mathop \smallint \limits_0^T f\left( t \right)\cos n{\omega _o}t;dt\)
\({a_1} = \frac{2}{T}\mathop \smallint \limits_0^T f\left( t \right){\rm{cost}}dt\)
\(= \frac{1}{\pi }\mathop \smallint \limits_0^T A\sin t\cos tdt\)
\(= \frac{A}{{2\pi }}\mathop \smallint \limits_0^T \sin 2t;dt = \frac{A}{{2\pi }}\mathop \smallint \limits_0^T \sin 2t;dt\)
=2πA[−2cos2t]0π=0
\({b_n} = \frac{2}{T}\mathop \smallint \limits_0^T f\left( t \right)\sin n\omega t;dt\)
\({b_1} = \frac{2}{{2\pi }}\mathop \smallint \limits_0^{2\pi } f\left( t \right)\sin tdt\)
\(= \frac{1}{\pi }\mathop \smallint \limits_0^\pi A\sin t\sin t;dt\)
\(= \frac{A}{\pi }\mathop \smallint \limits_0^\pi {\sin ^2}tdt\)
\(= \frac{A}{\pi }\mathop \smallint \limits_0^\pi A{\sin ^2}t;dt\)
\(= ;\frac{A}{\pi }\mathop \smallint \limits_0^\pi \frac{{1 - \cos 2t}}{2};dt\)
\(= \frac{A}{{2\pi }}\mathop \smallint \limits_0^\pi \left[ {t - \frac{{sin2t}}{2}} \right]_0^\pi\)
=2πA[(π−0)−(0−0)]=2A