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The Art of the Helicopter John Watkinson - Karatunov.net

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

<strong>the</strong> location in question is known, <strong>the</strong> error can be minimized by adjusting <strong>the</strong> altimeter<br />

setting scale to that pressure. However, if instead <strong>the</strong> altimeter setting scale is set to <strong>the</strong><br />

ISA MSL pressure <strong>of</strong> 1013.2 hPa, <strong>the</strong> altimeter reads pressure altitude. This is defined<br />

as <strong>the</strong> altitude in <strong>the</strong> ISA at which <strong>the</strong> same pressure exists. Pressure altitude is used<br />

primarily for flight in airways where it assures vertical separation (see section 7.7).<br />

Whereas pressure is primarily a navigational tool, density is what governs performance.<br />

Engines produce power by releasing <strong>the</strong>rmal energy due to combustion <strong>of</strong><br />

hydrocarbon fuel in air. <strong>The</strong> mass <strong>of</strong> fuel that can be burned is directly proportional<br />

to <strong>the</strong> mass <strong>of</strong> <strong>the</strong> air available, whereas physical limitations in <strong>the</strong> construction <strong>of</strong> <strong>the</strong><br />

engine set <strong>the</strong> greatest volume <strong>of</strong> air that can be drawn in. Consequently <strong>the</strong> density<br />

has a significant effect because it determines <strong>the</strong> mass <strong>of</strong> air per unit <strong>of</strong> volume <strong>the</strong><br />

engine has drawn in. Lift is obtained when <strong>the</strong> rotor imparts downward momentum to<br />

<strong>the</strong> air. As <strong>the</strong> disc area is fixed, <strong>the</strong> volume <strong>of</strong> air <strong>the</strong> rotor can influence is also fixed<br />

for a given flight regime. Thus <strong>the</strong> degree to which <strong>the</strong> rotor can impart momentum is<br />

controlled by air density.<br />

In <strong>the</strong> ISA <strong>the</strong> density at a given height will always be <strong>the</strong> same because ISA defines<br />

MSL pressure and temperature and specifies zero humidity. Thus using <strong>the</strong> standard<br />

figures, <strong>the</strong> pressure and temperature at any height can be deduced and <strong>the</strong> density must<br />

follow from that. In practice, <strong>the</strong> pressure and temperature will differ from ISA and <strong>the</strong><br />

local density will not be ISA density. <strong>The</strong> concept <strong>of</strong> density altitude was introduced to<br />

allow for such changes. Density altitude is <strong>the</strong> altitude in <strong>the</strong> ISA at which <strong>the</strong> density<br />

is <strong>the</strong> same as <strong>the</strong> present density. In order to assess <strong>the</strong> performance <strong>of</strong> a machine<br />

under real conditions, <strong>the</strong> pilot will calculate <strong>the</strong> density altitude for those conditions<br />

and <strong>the</strong>n consult <strong>the</strong> flight manual where <strong>the</strong> performance is specified as a function <strong>of</strong><br />

density altitude.<br />

Figure 8.1 shows a standard density/altitude chart that converts pressure altitude<br />

entered on <strong>the</strong> diagonal lines to density altitude measured along <strong>the</strong> vertical axis. <strong>The</strong><br />

horizontal axis is air temperature and <strong>the</strong> single line falling to <strong>the</strong> right shows <strong>the</strong> ISA<br />

air temperature falling with height at <strong>the</strong> standard lapse rate with pressure altitude.<br />

Thus <strong>the</strong> chart shows that <strong>the</strong> line corresponding to zero pressure altitude crosses <strong>the</strong><br />

line corresponding to zero density altitude at 15 ◦ C (ISA MSL conditions). In order to<br />

use <strong>the</strong> chart, <strong>the</strong> local pressure altitude is located where it crosses <strong>the</strong> ISA lapse rate<br />

line. Reading vertically down from this pressure altitude will give <strong>the</strong> ISA temperature<br />

for that height. If <strong>the</strong> actual temperature is <strong>the</strong> same, <strong>the</strong> pressure altitude and density<br />

altitude are <strong>the</strong> same. However, in practice a different temperature will <strong>of</strong>ten be found.<br />

If <strong>the</strong> diagonal line sloping from bottom left to top right and corresponding to <strong>the</strong><br />

pressure altitude is followed until it intersects a vertical line drawn up from <strong>the</strong> actual<br />

temperature, <strong>the</strong> vertical position <strong>of</strong> <strong>the</strong> intersection determines <strong>the</strong> density altitude.<br />

<strong>The</strong> figure shows an example. In some flight manuals, <strong>the</strong> conversion to density altitude<br />

may be incorporated in certain performance charts. An example will be given in <strong>the</strong><br />

next section.<br />

<strong>The</strong> effect <strong>of</strong> humidity is not generally considered in density altitude charts, but a rule<br />

<strong>of</strong> thumb used by pilots is to add 1000 feet to <strong>the</strong> density altitude if <strong>the</strong> humidity is<br />

high. Typically helicopters have no means to measure humidity and <strong>the</strong> pilot’s estimate<br />

has to be used.<br />

8.5 Power management<br />

<strong>Helicopter</strong> operation is largely concerned with power management. <strong>The</strong> power plant<br />

supplies power and <strong>the</strong> airframe demands power. Both supply and demand are

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