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The Art of the Helicopter John Watkinson - Karatunov.net

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Technical background 47<br />

Fig. 2.28 Fourier analysis allows <strong>the</strong> syn<strong>the</strong>sis <strong>of</strong> any waveform by <strong>the</strong> addition <strong>of</strong> discrete frequencies <strong>of</strong><br />

appropriate amplitude and phase.<br />

by creating all <strong>of</strong> <strong>the</strong> right harmonics and adding <strong>the</strong>m is called an inverse transform.<br />

Figure 2.29 shows how a square wave can be syn<strong>the</strong>sized in this way by adding toge<strong>the</strong>r<br />

different harmonics <strong>of</strong> <strong>the</strong> correct amplitude and phase.<br />

Fourier analysis is based on multiplying <strong>the</strong> waveform to be analysed by sine waves<br />

called ‘basis functions’. In order to analyse an arbitrary waveform to see if it contains<br />

a particular frequency, it is multiplied by a basis function at that frequency and <strong>the</strong><br />

product is averaged. Figure 2.30(a) shows that if <strong>the</strong> signal being analysed contains a<br />

component having <strong>the</strong> same frequency as that <strong>of</strong> <strong>the</strong> basis function <strong>the</strong> product will have<br />

a zero frequency component that will give a finite result after averaging. <strong>The</strong> value <strong>of</strong><br />

<strong>the</strong> result after averaging is called a coefficient. Components at all o<strong>the</strong>r frequencies will<br />

average to zero. Thus a complete Fourier analysis requires <strong>the</strong> process to be repeated<br />

at all <strong>of</strong> <strong>the</strong> frequencies <strong>of</strong> interest.<br />

Figure 2.30(c) shows that if by chance <strong>the</strong> input and <strong>the</strong> basis function have a phase<br />

difference <strong>of</strong> 90 ◦ <strong>the</strong> product will be zero even though <strong>the</strong> frequencies are identical.

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