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The Art of the Helicopter John Watkinson - Karatunov.net

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Technical background 45<br />

<strong>the</strong> cosine components will be in anti-phase and will cancel. Thus all real frequencies<br />

actually contain equal amounts <strong>of</strong> positive and negative frequencies. <strong>The</strong>se cannot be<br />

distinguished unless a modulation process takes place. Figure 2.25(b) shows that when<br />

two signals <strong>of</strong> frequency ±ω1 and ±ω2, are multiplied toge<strong>the</strong>r, <strong>the</strong> result is that <strong>the</strong><br />

rotations <strong>of</strong> each must be added. <strong>The</strong> result is four frequencies, ±(ω1 +ω2) and ±(ω1 −<br />

ω2), one <strong>of</strong> which is <strong>the</strong> sum <strong>of</strong> <strong>the</strong> input frequencies and one <strong>of</strong> which is <strong>the</strong> difference<br />

between <strong>the</strong>m. <strong>The</strong>se are called sidebands. Sidebands are found extensively in avionics,<br />

where <strong>the</strong> deliberate use <strong>of</strong> <strong>the</strong> process is called heterodyning. In a communications<br />

radio <strong>the</strong> carrier frequency is multiplied or ‘modulated’ by <strong>the</strong> audio speech signal,<br />

called <strong>the</strong> baseband signal, and <strong>the</strong> result is a pair <strong>of</strong> sidebands above and below <strong>the</strong><br />

carrier.<br />

<strong>The</strong> rotation <strong>of</strong> <strong>the</strong> helicopter rotor has a certain frequency. Any vibration due to<br />

periodic motion affecting <strong>the</strong> movement <strong>of</strong> <strong>the</strong> blades within <strong>the</strong> rotor plane may have<br />

a characteristic frequency with respect to <strong>the</strong> rotor. When referred to <strong>the</strong> hull <strong>of</strong> <strong>the</strong><br />

helicopter, <strong>the</strong> frequency <strong>of</strong> <strong>the</strong> vibration may have been heterodyned by <strong>the</strong> rotor<br />

frequency and <strong>the</strong> frequencies experienced in <strong>the</strong> hull may <strong>the</strong>n be <strong>the</strong> frequencies <strong>of</strong><br />

<strong>the</strong> sidebands. This will be considered in Chapters 3 and 4.<br />

In a voice radio system, <strong>the</strong> carrier frequency is much higher than <strong>the</strong> frequencies in<br />

<strong>the</strong> speech, whereas in o<strong>the</strong>r systems this may not be <strong>the</strong> case. In digital systems, continuous<br />

signals are represented by periodic measurements, or samples, and sidebands are<br />

found above and below <strong>the</strong> frequency <strong>of</strong> <strong>the</strong> sampling clock Fs. Figure 2.26(a) shows<br />

<strong>the</strong> spectrum <strong>of</strong> a sampling clock which contains harmonics because it is a pulse train<br />

not a sinusoid. Figure 2.26(b) shows that <strong>the</strong> sidebands <strong>of</strong> <strong>the</strong> sampling frequency can<br />

be rejected using a low-pass filter which allows through only <strong>the</strong> original baseband<br />

signal. <strong>The</strong> sampled representation <strong>of</strong> <strong>the</strong> signal is returned to a continuous waveform.<br />

This is exactly what happens in a Compact Disc player.<br />

As <strong>the</strong> baseband frequency rises, <strong>the</strong> lower sideband frequency must fall. However,<br />

this can only continue until <strong>the</strong> base bandwidth is half <strong>the</strong> sampling rate. This is known<br />

as <strong>the</strong> Nyquist frequency and it represents <strong>the</strong> highest baseband frequency at which<br />

<strong>the</strong> original signal can be recovered by a low-pass filter.<br />

Fig. 2.26 (a) Spectrum <strong>of</strong> sampling pulses. (b) Spectrum <strong>of</strong> samples. (c) Aliasing due to sideband overlap.

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