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The Art of the Helicopter John Watkinson - Karatunov.net

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Introduction to helicopter dynamics 65<br />

Clearly such a wing will be creating a lot <strong>of</strong> drag at <strong>the</strong> small angles <strong>of</strong> attack needed<br />

at high speeds. For high speed operation, <strong>the</strong> camber will need to be very small, but<br />

this kind <strong>of</strong> wing will be inefficient if used at large angles <strong>of</strong> attack at low speed, hence<br />

<strong>the</strong> use <strong>of</strong> flaps on fixed-wing aircraft. With a cambered section, air is still accelerated<br />

downwards leaving <strong>the</strong> section even when <strong>the</strong> angle <strong>of</strong> attack is zero, and so a slight<br />

negative angle <strong>of</strong> attack is necessary to obtain <strong>the</strong> zero lift condition.<br />

Figure 3.3(b) shows a symmetrical section in which <strong>the</strong> camber line and <strong>the</strong> chord line<br />

are one and <strong>the</strong> same. A symmetrical section is a streamlined flat plate. <strong>The</strong> curvature<br />

prevents separation over <strong>the</strong> leading edge. At zero angle <strong>of</strong> attack, <strong>the</strong> airflow is also<br />

symmetrical, and no <strong>net</strong> air reaction results. <strong>The</strong>re is thus no induced drag, only pr<strong>of</strong>ile<br />

drag. If <strong>the</strong> angle <strong>of</strong> attack is made positive, air is accelerated down, and <strong>the</strong> reaction is<br />

upwards. If <strong>the</strong> angle <strong>of</strong> attack is made negative, air is accelerated up and <strong>the</strong> reaction<br />

is downwards.<br />

<strong>The</strong> reader is cautioned against explanations <strong>of</strong> <strong>the</strong> origin <strong>of</strong> lift based on Bernouilli’s<br />

<strong>the</strong>orem. Bernouilli made it quite clear that his <strong>the</strong>orem relates to conservation <strong>of</strong><br />

energy in flowing air such that <strong>the</strong> sum <strong>of</strong> <strong>the</strong> static and dynamic pressures remains<br />

constant. Bernouilli’s <strong>the</strong>orem only applies if no energy is put into <strong>the</strong> air. However, a<br />

wing or a rotor blade is an actuator that is exchanging energy with <strong>the</strong> air. This is clear<br />

from <strong>the</strong> presence <strong>of</strong> induced drag. When energy is put into <strong>the</strong> airflow, Bernouilli’s<br />

<strong>the</strong>orem simply doesn’t apply and <strong>the</strong> explanations based on it are flawed and should<br />

be disregarded.<br />

3.2 <strong>The</strong> centre <strong>of</strong> pressure<br />

<strong>The</strong> lift developed by <strong>the</strong> blades is distributed over <strong>the</strong> chord, but not uniformly. <strong>The</strong><br />

centre <strong>of</strong> pressure is where a single force would act producing <strong>the</strong> same effect as <strong>the</strong><br />

distributed lift. In real airfoil sections, <strong>the</strong> centre <strong>of</strong> pressure is ahead <strong>of</strong> <strong>the</strong> mid-chord<br />

point. If <strong>the</strong> blade is made <strong>of</strong> a material with uniform density, <strong>the</strong> centre <strong>of</strong> pressure<br />

will be ahead <strong>of</strong> <strong>the</strong> centre <strong>of</strong> mass and, as Figure 3.4(a) shows, a couple results. This<br />

couple would tend to twist <strong>the</strong> blade and increase <strong>the</strong> angle <strong>of</strong> attack, making <strong>the</strong> lift<br />

greater and increasing <strong>the</strong> twist fur<strong>the</strong>r. In extreme cases <strong>the</strong> blade will flutter; a violent<br />

condition that will usually destroy any structure suffering from it.<br />

In aircraft, wings can usually be made rigid enough to prevent flutter, but this cannot<br />

be done with <strong>the</strong> long thin blades <strong>of</strong> <strong>the</strong> helicopter. <strong>The</strong> solution universally adopted is<br />

to construct <strong>the</strong> blade so that <strong>the</strong> mass centroid (see Chapter 2) <strong>of</strong> <strong>the</strong> blade is ahead <strong>of</strong><br />

Couple Couple<br />

(a) (b)<br />

Fig. 3.4 (a) If <strong>the</strong> centre <strong>of</strong> lift is ahead <strong>of</strong> <strong>the</strong> CM, lift tends to increase <strong>the</strong> angle <strong>of</strong> attack. (b) If <strong>the</strong> centre <strong>of</strong><br />

lift is behind <strong>the</strong> CM, lift tends to reduce <strong>the</strong> angle <strong>of</strong> attack: a stable condition.

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