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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<strong>Helicopter</strong> performance 325<br />
column is proportional to pressure and can be expressed in inches or cm <strong>of</strong> mercury. At<br />
sea level a reading <strong>of</strong> about 26 inches <strong>of</strong> mercury is obtained. This unit may be found<br />
in use in altimeters originating in <strong>the</strong> United States.<br />
<strong>The</strong> gas law states that <strong>the</strong> product <strong>of</strong> pressure and volume is proportional to temperature.<br />
Reducing <strong>the</strong> volume means that external work has to be done to oppose <strong>the</strong> pressure.<br />
This work increases <strong>the</strong> temperature <strong>of</strong> <strong>the</strong> gas. <strong>The</strong> Diesel engine obtains ignition<br />
in this way. Conversely if <strong>the</strong> volume is increased, work is done by <strong>the</strong> gas and <strong>the</strong> temperature<br />
must fall. This is why carburettors are prone to icing on part throttle because<br />
<strong>the</strong> air expands on entering <strong>the</strong> manifold. Air conditioners work in <strong>the</strong> same way.<br />
If <strong>the</strong> volume is fixed, as temperature rises, <strong>the</strong> velocity <strong>of</strong> <strong>the</strong> molecules increases<br />
and so <strong>the</strong> impact at each collision with <strong>the</strong> walls <strong>of</strong> any container is greater and <strong>the</strong><br />
pressure rises. Alternatively <strong>the</strong> same pressure can be exerted in a given volume with<br />
a smaller mass <strong>of</strong> gas. Thus in <strong>the</strong> atmosphere where pressure increases can be released<br />
by free movement, <strong>the</strong> result <strong>of</strong> an increase in air temperature is that <strong>the</strong> density goes<br />
down. Density is also affected by humidity. Water molecules are heavier than those <strong>of</strong><br />
atmospheric gases and increase <strong>the</strong> pressure due to molecular collisions. Thus in <strong>the</strong><br />
presence <strong>of</strong> water vapour a given pressure can be sustained with a smaller mass <strong>of</strong> air<br />
and <strong>the</strong> density goes down.<br />
8.3 International Standard Atmosphere<br />
In order for meaningful comparisons to be made between various test results, it is<br />
important to eliminate variations due to atmospheric conditions. <strong>The</strong> International<br />
Standard Atmosphere (ISA) is a defined set <strong>of</strong> fixed conditions, somewhere within <strong>the</strong><br />
spread <strong>of</strong> conditions found in practice. When a test is made, <strong>the</strong> actual atmospheric<br />
conditions are measured. Using <strong>the</strong> laws <strong>of</strong> physics, it is possible to calculate <strong>the</strong> effect<br />
<strong>of</strong> every difference between <strong>the</strong> actual conditions and ISA. If all results are corrected in<br />
this way, <strong>the</strong>y can be presented with respect to ISA and as a result can immediately be<br />
compared with any o<strong>the</strong>r results obtained in <strong>the</strong> same way. Similarly, if <strong>the</strong> performance<br />
<strong>of</strong> a machine is defined in <strong>the</strong> flight manual with respect to ISA, it is possible to correct<br />
for <strong>the</strong> actual conditions and predict <strong>the</strong> real performance that can be expected.<br />
In <strong>the</strong> ISA, pressure and temperature at mean sea level (MSL) are defined, along<br />
with standardized rates at which <strong>the</strong>se change with height. Relative humidity (RH) is<br />
also defined to be zero. ISA MSL pressure is 1013.2 hPa. Temperature is 15 ◦ C and<br />
<strong>the</strong> density is 1.225 kg/m 3 . <strong>The</strong> ISA lapse rate defines temperature as falling at 1.98 ◦ C<br />
per 1000 feet (which is a mongrel unit being part metric and part imperial). Although<br />
<strong>the</strong> height <strong>of</strong> <strong>the</strong> tropopause is a function <strong>of</strong> latitude because <strong>the</strong> earth is rotating, ISA<br />
defines <strong>the</strong> tropopause as 36 000 feet and above this <strong>the</strong> air temperature is −56.5 ◦ C. For<br />
many purposes <strong>the</strong> approximation <strong>of</strong> −2 ◦ C per 1000 feet can be used as <strong>the</strong> lapse rate.<br />
Given <strong>the</strong> above, <strong>the</strong> pressure and density <strong>of</strong> <strong>the</strong> ISA can be calculated for any height<br />
above sea level. <strong>The</strong> density is important because it directly affects <strong>the</strong> power that can<br />
be produced by <strong>the</strong> engine(s) and <strong>the</strong> thrust produced by <strong>the</strong> rotors.<br />
8.4 Pressure and density altitude<br />
Altimeters do not measure height because <strong>the</strong>y are basically pressure gauges with<br />
a creative scale. Only in ISA conditions does an altimeter measure height because <strong>the</strong><br />
pressure will correctly match <strong>the</strong> scale reading. In all o<strong>the</strong>r conditions, <strong>the</strong> altimeter<br />
reads altitude, best defined as estimated height subject to an error. If sea level pressure at