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
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
68 <strong>The</strong> <strong>Art</strong> <strong>of</strong> <strong>the</strong> <strong>Helicopter</strong><br />
A rotor hovering at L/Dmax. has a load factor <strong>of</strong> unity and would stall in any real<br />
manoeuvre. It is thus a characteristic <strong>of</strong> helicopters that <strong>the</strong> rotor must operate below<br />
L/Dmax. <strong>of</strong> <strong>the</strong> blade section in <strong>the</strong> hover in order to allow a reasonable load factor for<br />
forward flight.<br />
Turning at a given rate (number <strong>of</strong> degrees per second) requires a lateral acceleration<br />
proportional to <strong>the</strong> square <strong>of</strong> <strong>the</strong> airspeed. As aeroplanes tend to fly faster than helicopters,<br />
<strong>the</strong>y will need high load factors to obtain reasonable rates <strong>of</strong> turn. Aeroplanes<br />
automatically have high load factors at speed because available lift increases as <strong>the</strong><br />
square <strong>of</strong> <strong>the</strong> airspeed. In helicopters lift is dominated by rotor speed, not airspeed<br />
and so load factors in helicopters tend to be small although helicopters can still easily<br />
out-turn most aeroplanes.<br />
As <strong>the</strong> relative airflow in helicopters is dominated by <strong>the</strong> rotor speed, <strong>the</strong> gust response<br />
<strong>of</strong> helicopters is much reduced in comparison to that <strong>of</strong> aeroplanes. This is one reason<br />
why helicopters can operate in bad wea<strong>the</strong>r. A fur<strong>the</strong>r small luxury is that <strong>the</strong> flexibility<br />
<strong>of</strong> <strong>the</strong> rotor gives in gusts a decoupling effect similar to that given by <strong>the</strong> suspension<br />
<strong>of</strong> a car.<br />
3.4 Collective control<br />
In a hovering helicopter, <strong>the</strong> only source <strong>of</strong> lift is <strong>the</strong> rotor. Obtaining sufficient lift is<br />
only a matter <strong>of</strong> providing a suitable combination <strong>of</strong> power and efficiency, and is much<br />
easier than controlling lift. As <strong>the</strong> lift is proportional to <strong>the</strong> square <strong>of</strong> <strong>the</strong> speed, it is<br />
in principle possible to control lift by changing <strong>the</strong> rotor speed. Some early machines<br />
did just that. Unfortunately, <strong>the</strong> inertia <strong>of</strong> <strong>the</strong> rotor means that speed changes cannot<br />
rapidly be accomplished. For practical reasons a constant rotor speed is much to be<br />
preferred.<br />
<strong>The</strong> proportionality between <strong>the</strong> coefficient <strong>of</strong> lift and <strong>the</strong> angle <strong>of</strong> attack is <strong>the</strong><br />
solution. As was shown in Figure 3.1, <strong>the</strong> rotor blades are mounted on fea<strong>the</strong>ring<br />
bearings. Figure 1.21 showed that <strong>the</strong> pilot holds in his left hand a collective pitch<br />
lever pivoted near <strong>the</strong> back <strong>of</strong> his seat. <strong>The</strong> lever gets its name because by lifting it,<br />
<strong>the</strong> pitch angle <strong>of</strong> all <strong>of</strong> <strong>the</strong> rotor blades is increased by <strong>the</strong> same amount, and <strong>the</strong><br />
rotor lift increases immediately. This feature <strong>of</strong> <strong>the</strong> helicopter contributes enormously<br />
to its safety. When a fixed-wing aircraft flies slowly, sudden loss <strong>of</strong> lift can only be<br />
countered by raising <strong>the</strong> airspeed and this takes time. In <strong>the</strong> helicopter <strong>the</strong> airspeed is<br />
always present due to <strong>the</strong> rotating blades and as this speed is many times higher than<br />
any normal windspeed, <strong>the</strong> airspeed seen by <strong>the</strong> blades is always adequate.<br />
In addition to instantaneous response to changing lift conditions, <strong>the</strong> helicopter rotor<br />
stores in ki<strong>net</strong>ic energy <strong>the</strong> equivalent <strong>of</strong> full engine power applied for several seconds.<br />
<strong>The</strong> pilot can transiently increase <strong>the</strong> available power by using so much collective pitch<br />
that <strong>the</strong> rotor slows down and converts its ki<strong>net</strong>ic energy into lift.<br />
3.5 In <strong>the</strong> hover<br />
Figure 3.6(a) shows a helicopter with flight RRPM, but with <strong>the</strong> collective lever lowered.<br />
<strong>The</strong> thrust vector is small, so gravity keeps <strong>the</strong> machine firmly on <strong>the</strong> ground. If <strong>the</strong><br />
collective lever is raised, eventually <strong>the</strong> rotor thrust vector will exceed <strong>the</strong> weight, and<br />
<strong>the</strong> machine will rise. By adjusting <strong>the</strong> collective lever, <strong>the</strong> machine can be made to<br />
hover with <strong>the</strong> thrust exactly balancing <strong>the</strong> weight as in (b). If <strong>the</strong> thrust is directly