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The Art of the Helicopter John Watkinson - Karatunov.net

The Art of the Helicopter John Watkinson - Karatunov.net

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Introduction to helicopter dynamics 93<br />

Fig. 3.25 How <strong>the</strong> cyclic stick might be trimmed at different airspeeds. Inflow roll begins at low airspeed but<br />

has less effect as speed rises, whereas coning roll increases with speed as <strong>the</strong> coning angle may increase to<br />

produce more thrust.<br />

with airspeed. Figure 3.25 shows how <strong>the</strong> lateral cyclic control might have to be moved<br />

to <strong>the</strong> retreating side in order to fly straight at different airspeeds.<br />

Thus in straight flight at constant speed, <strong>the</strong> cyclic stick must be held slightly towards<br />

<strong>the</strong> retreating side to counteract <strong>the</strong> inflow and coning induced rolls as well as forwards<br />

to counter <strong>the</strong> advancing/retreating induced pitch-up. In some machines <strong>the</strong> phasing <strong>of</strong><br />

<strong>the</strong> controls is arranged so that forward cyclic automatically creates a degree <strong>of</strong> lateral<br />

cyclic. However, in <strong>the</strong> hover this results in <strong>the</strong> machine not responding precisely in <strong>the</strong><br />

direction <strong>the</strong> stick is pushed.<br />

Like <strong>the</strong> collective control, <strong>the</strong>re is no one correct setting for <strong>the</strong> cyclic control. <strong>The</strong><br />

cyclic trim control is used to shift <strong>the</strong> neutral position <strong>of</strong> <strong>the</strong> stick, relieving <strong>the</strong> pilot<br />

<strong>of</strong> <strong>the</strong> need to produce continuous control forces.<br />

3.22 Rotor H-force<br />

<strong>The</strong> retreating blade has <strong>the</strong> airspeed subtracted from <strong>the</strong> rotational speed and so has<br />

to operate with an increased angle <strong>of</strong> attack. <strong>The</strong> pr<strong>of</strong>ile drag will be reduced but<br />

<strong>the</strong> induced drag will increase. Conversely <strong>the</strong> advancing blade will suffer significantly<br />

more pr<strong>of</strong>ile drag because <strong>of</strong> <strong>the</strong> high relative airspeed, but <strong>the</strong> induced drag will fall<br />

because <strong>the</strong> angle <strong>of</strong> attack has been reduced. <strong>The</strong> overall effect <strong>of</strong> pr<strong>of</strong>ile drag and<br />

induced drag does not balance between <strong>the</strong> advancing and retreating sides and <strong>the</strong><br />

resultant is a rearward acting force called <strong>the</strong> H-force. Figure 3.26 shows that <strong>the</strong><br />

H-force is <strong>the</strong> reason why <strong>the</strong> rotor thrust is not precisely at right angles to <strong>the</strong> tip path<br />

plane. A typical figure is 1 ◦ .<br />

Because <strong>of</strong> inflow and coning, <strong>the</strong> blades crossing <strong>the</strong> nose produce more lift than<br />

<strong>the</strong> blades crossing <strong>the</strong> tail and so <strong>the</strong> induced drag is not <strong>the</strong> same. <strong>The</strong> resultant is <strong>the</strong><br />

Y-force which acts at right angles to <strong>the</strong> direction <strong>of</strong> flight. <strong>The</strong> H-force is small and<br />

<strong>the</strong> Y-force is very small with <strong>the</strong> result that <strong>the</strong> effect on <strong>the</strong> magnitude <strong>of</strong> <strong>the</strong> thrust<br />

is insignificant.<br />

3.23 Blade stall and compressibility<br />

Stall occurs when air passing over <strong>the</strong> cambered upper surface <strong>of</strong> a blade can no longer<br />

accelerate rapidly enough to follow <strong>the</strong> surface. Airflow breaks away and lift is lost

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