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The Art of the Helicopter John Watkinson - Karatunov.net

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36 <strong>The</strong> <strong>Art</strong> <strong>of</strong> <strong>the</strong> <strong>Helicopter</strong><br />

Fig. 2.15 Wavelength is defined as <strong>the</strong> distance between two points at <strong>the</strong> same place on adjacent cycles.<br />

Wavelength is inversely proportional to frequency.<br />

Because sound travels at a finite speed, <strong>the</strong> fixed observer at some distance from <strong>the</strong><br />

source will experience <strong>the</strong> disturbance at some later time. In <strong>the</strong> case <strong>of</strong> a transient, <strong>the</strong><br />

observer will detect a single replica <strong>of</strong> <strong>the</strong> original as it passes at <strong>the</strong> speed <strong>of</strong> sound.<br />

In <strong>the</strong> case <strong>of</strong> <strong>the</strong> tuning fork, a periodic sound source, <strong>the</strong> pressure peaks and dips<br />

follow one ano<strong>the</strong>r away from <strong>the</strong> source at <strong>the</strong> speed <strong>of</strong> sound. For a given rate <strong>of</strong><br />

vibration <strong>of</strong> <strong>the</strong> source, a given peak will have propagated a constant distance before<br />

<strong>the</strong> next peak occurs. This distance is called <strong>the</strong> wavelength lambda. Figure 2.15 shows<br />

that wavelength is defined as <strong>the</strong> distance between any two identical points on <strong>the</strong><br />

whole cycle. If <strong>the</strong> source vibrates faster, successive peaks get closer toge<strong>the</strong>r and <strong>the</strong><br />

wavelength gets shorter. <strong>The</strong> wavelength is inversely proportional to <strong>the</strong> frequency.<br />

It is easy to remember that <strong>the</strong> wavelength <strong>of</strong> 1000 Hz is a foot (about 30 cm) at sea<br />

level.<br />

2.11 <strong>The</strong> mechanics <strong>of</strong>oscillation<br />

By definition helicopters contain a lot <strong>of</strong> rotating parts and for a proper understanding<br />

<strong>of</strong> <strong>the</strong>ir characteristics, knowledge <strong>of</strong> <strong>the</strong> mechanics <strong>of</strong> rotation is essential. In physics,<br />

<strong>the</strong> engineering quantity <strong>of</strong> RPM is not used. Instead <strong>the</strong> unit <strong>of</strong> angular velocity is<br />

radians per second and <strong>the</strong> symbol used is ω. Figure 2.16 shows that a radian is a<br />

natural unit <strong>of</strong> angle which is <strong>the</strong> angle subtended by unit circumference at unit radius.<br />

As <strong>the</strong> circumference is given by 2π times <strong>the</strong> radius, <strong>the</strong>n <strong>the</strong>re will be 2π radians in<br />

one revolution, such that one radian is about 57 ◦ .<br />

Figure 2.17 shows a constant speed rotation viewed along <strong>the</strong> axis so that <strong>the</strong> motion<br />

is circular. Imagine, however, <strong>the</strong> view from one side in <strong>the</strong> plane <strong>of</strong> <strong>the</strong> rotation. From a<br />

distance, only a vertical oscillation will be observed and if <strong>the</strong> position is plotted against<br />

time <strong>the</strong> resultant waveform will be a sine wave. <strong>The</strong> sine wave is unique because it<br />

contains only a single frequency. All o<strong>the</strong>r waveforms contain more than one frequency.<br />

Imagine a second viewer who is at right angles to <strong>the</strong> first viewer. He will observe<br />

<strong>the</strong> same waveform, but at a different time. <strong>The</strong> displacement is given by multiplying<br />

<strong>the</strong> radius by <strong>the</strong> cosine <strong>of</strong> <strong>the</strong> phase angle. When plotted on <strong>the</strong> same graph, <strong>the</strong> two<br />

waveforms are phase shifted with respect to one ano<strong>the</strong>r. In this case <strong>the</strong> phase shift is<br />

90 ◦ and <strong>the</strong> two waveforms are said to be in quadrature. Incidentally <strong>the</strong> motions on<br />

each side <strong>of</strong> a steam locomotive are in quadrature so that it can always get started (<strong>the</strong><br />

term used is quartering). Note that <strong>the</strong> phase angle <strong>of</strong> a signal is constantly changing<br />

with time whereas <strong>the</strong> phase shift between two signals can be constant. It is important<br />

that <strong>the</strong>se two are not confused. In a three-bladed rotor, <strong>the</strong> motion <strong>of</strong> each blade

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