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Figure 3


Fig. 3 Fourier series for g(t). A complicated wave g(t) can be rewritten as an infinite sum of simple cosine and sine waves by progressively increasing their fundamental frequency f by integers n, and by varying their amplitudes, an and bn. If we substitute g(t) = 1 (a square wave) into the equations shown here, we obtain expressions for a0, an, and bn that can be inserted into the Fourier series. After simplifying, we are left with a Fourier approximation for a square wave.