The Art of the Helicopter John Watkinson - Karatunov.net
The Art of the Helicopter John Watkinson - Karatunov.net
The Art of the Helicopter John Watkinson - Karatunov.net
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108 <strong>The</strong> <strong>Art</strong> <strong>of</strong> <strong>the</strong> <strong>Helicopter</strong><br />
incorporate electronic systems and sensors used ei<strong>the</strong>r to control or navigate <strong>the</strong><br />
machine or as part <strong>of</strong> its mission equipment. Electronic equipment does not take<br />
kindly to vibration, or if specially adapted, must be more expensive.<br />
Vibrating masses are a common origin <strong>of</strong> sound, so it follows that a vibrating helicopter<br />
will be noisy both inside and out. External noise causes disturbance in civil<br />
operations and may compromise military missions. A significant part <strong>of</strong> <strong>the</strong> design process<br />
<strong>of</strong> <strong>the</strong> modern helicopter is taken up in minimizing noise and vibration. <strong>The</strong>re are a<br />
number <strong>of</strong> approaches that will be combined in various ways. Study <strong>of</strong> <strong>the</strong> aerodynamic<br />
origins <strong>of</strong> vibration may allow a reduction at <strong>the</strong> source. Once <strong>the</strong> forcing frequencies<br />
are known, <strong>the</strong> design <strong>of</strong> <strong>the</strong> structure should ensure that resonant responses to those<br />
frequencies are minimized. This is known as detuning. Vibration may be isolated or<br />
decoupled in some way, damped using lossy materials to convert flexing into heat, or<br />
opposed or absorbed through various cancelling techniques, both passive and active.<br />
<strong>The</strong> reduction <strong>of</strong> <strong>the</strong> vibration at source has to be <strong>the</strong> technically superior solution.<br />
<strong>The</strong> disadvantage <strong>of</strong> decoupling <strong>the</strong> vibration from <strong>the</strong> passengers is that although <strong>the</strong>ir<br />
comfort is improved, <strong>the</strong> vibration experienced by <strong>the</strong> parts that are not decoupled<br />
may actually increase. It is easy to see why. For a given exciting force, <strong>the</strong> amplitude<br />
<strong>of</strong> a vibration is inversely proportional to <strong>the</strong> mass being vibrated. In a conventional<br />
helicopter <strong>the</strong> dominant masses are those <strong>of</strong> <strong>the</strong> transmission, hull and payload. If <strong>the</strong><br />
hull and payload are decoupled, <strong>the</strong> mass seen by <strong>the</strong> vibration source is now only that<br />
<strong>of</strong> <strong>the</strong> transmission and <strong>the</strong> amplitude <strong>of</strong> <strong>the</strong> vibration <strong>the</strong>re must be greater and not<br />
necessarily beneficial.<br />
An obvious way <strong>of</strong> reducing vibration at source is to use non-sinusoidal cyclic pitch<br />
control that allows <strong>the</strong> lift moment to be more nearly constant as <strong>the</strong> blade turns.<br />
<strong>The</strong> means to do this are non-trivial and are described in section 3.28. Ano<strong>the</strong>r way<br />
<strong>of</strong> reducing vibration is to use more blades. This has several advantages. First, <strong>the</strong><br />
load on each blade is reduced and with it <strong>the</strong> magnitude <strong>of</strong> <strong>the</strong> forcing function <strong>of</strong><br />
each blade. Second, <strong>the</strong> more blades, <strong>the</strong> higher <strong>the</strong> frequency <strong>of</strong> <strong>the</strong> vibration will be<br />
and <strong>the</strong> lower will be <strong>the</strong> amplitude for a given mass. Figure 3.37 shows that a threebladed<br />
rotor eliminates <strong>the</strong> 2P hop <strong>of</strong> <strong>the</strong> two-bladed rotor, whereas a four-bladed rotor<br />
reintroduces some 2P lateral vibration. It will be seen from Figure 3.38(b) that an even<br />
number <strong>of</strong> blades gives lower rocking frequencies, making an odd number preferable.<br />
Consequently <strong>the</strong> change from four to five blades gives a significant improvement. Large<br />
transport helicopters inevitably have a large and generally odd number <strong>of</strong> blades – seven<br />
or nine – simply to contain <strong>the</strong> large vibrations that must result from generating high<br />
rotor thrust. Using many blades will be expensive and result in a large rotor head having<br />
high drag.<br />
It is common to design <strong>the</strong> blades so that <strong>the</strong>ir natural frequencies <strong>of</strong> vibration are<br />
not in <strong>the</strong> spectrum <strong>of</strong> <strong>the</strong> excitation. If any <strong>of</strong> <strong>the</strong> excitation frequencies coincide<br />
with <strong>the</strong> resonant frequencies <strong>the</strong>re could be a significant response at that frequency.<br />
Any coincidence can be seen from an interference diagram as shown in Figure 3.39.<br />
This interference diagram is for <strong>the</strong> Westland Lynx and shows <strong>the</strong> operating speed<br />
(318 RPM) as a vertical line. <strong>The</strong> excitation frequency may be at any integer multiple<br />
<strong>of</strong> <strong>the</strong> rotor frequency. Figure 3.39 shows that, as rotor speed increases, <strong>the</strong> excitation<br />
harmonics (thin lines starting at <strong>the</strong> origin) fan out. <strong>The</strong> resonant frequencies <strong>of</strong> <strong>the</strong><br />
blades also change with rotor frequency because <strong>of</strong> <strong>the</strong> effect <strong>of</strong> centrifugal stiffening.<br />
Figure 3.39 shows how flapping, ωf , and lagging, ωl, resonant frequencies may change<br />
with rotor speed.<br />
<strong>The</strong> only coincidence between excitation and response is <strong>the</strong> close correspondence<br />
between <strong>the</strong> fundamental flapping resonant frequency and <strong>the</strong> rotor fundamental frequency.<br />
This is <strong>the</strong> characteristic that results in rotor precession. Note that as <strong>the</strong> Lynx