Aircraft Performance
Factors Affecting Performance
Performance of the aircraft depends on the density of the air in which it
flies.
Factors affecting air density are:
- Barometric pressure
- Altitude
- Temperature
- Humidity
Standard Atmosphere Definition
The International Standards Association (ISA) has defined a Standard
Atmosphere as:
- Sea Level Barometric Pressure of 29.92 inches of Mercury (in. Hg)
- Sea Level Temperature of 15° Celsius (15° C or 59° F)
- Relative humidity of 0 %
- Standard temperature lapse rate of 2° C per 1000 feet altitude
- Standard pressure lapse rate of 1 in. Hg per 1000 feet altitude
- A standard decrease in density as altitude increases
The standard atmosphere definition provides a means for instrument and aircraft
manufacturers to specify the performance of their products in a uniform
way. This definition was arrived at by studying the average sea level pressure
and temperature over a number of years, seasons, and locations around the
world.
Seldom will an aircraft be in standard atmosphere conditions. In order to
define performance of an instrument or an aircraft in a non-standard atmosphere,
conversions must be applied to adjust the readings or performance numbers
to agree with the standard atmosphere. This adjustment is called Density
Altitude, and will be more fully defined later in this section.
Effects of Nonstandard Air Density
Air Density decreases:
- With Air Temperature Increase
- With Altitude Increase
- With Humidity Increase
- With Barometric Pressure Decrease
With lower air density:
- The engine develops less power.
- The propeller produces less thrust.
- The wings produce less lift.
This results in:
- Longer takeoff run
- Poorer climb performance
- Longer landing distance
Density Altitude
Density altitude is a way of relating the density of the air you are
in compared to the standard atmosphere. Three atmospheres are illustrated.
The Standard Atmosphere (29.92 in. Hg and 15 degrees Celsius) in middle
shown in gray. A less dense atmosphere (A ) (lower pressure and/or Higher
Temperature) is shown on the right in red. A more dense atmosphere (B)
(higher pressure and/or Colder Temperature) is illustrated on the left
in blue.
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If you are at an actual (true) altitude at location
A in atmosphere (A) (the red atmosphere on the right), you will
have to go to altitude (A') in the Standard Atmosphere to find the
same air density. This altitude in the standard atmosphere at (A')
is called the DENSITY ALTITUDE.
Similarly, if you are at atmosphere (B) (colder or
high pressure shown as blue on the left) the air will be more dense
than standard. Therefore you will have to go down to a lower actual
altitude in the standard atmosphere at (B') to find the equivalent
air density. This equivalent altitude in the Standard Atmosphere
is the DENSITY ALTITUDE.
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The reason that you need to convert
your actual nonstandard altitude (and thus your nonstandard air density)
to the standard density altitude is that all performance charts and data
is based on a standard atmosphere. For example, if you are at a high altitude
runway already, and the atmosphere pressure is low and temperature is high,
it will require a significantly longer take off run than you
may be accustomed to at your lower home base. If you are not aware of the
effects of density altitude on your aircraft performance, it could lead
to serious consequences.
Density Altitude Calculations
Density Altitude can be found in two ways
- Using conversion charts
- Using the E6B Flight Computer
Density Altitude calculation is a 2 step process.
Step 1. Find Pressure Altitude
Pressure Altitude adjusts for pressure difference between your air and
standard atmosphere. The question is “What would your altimeter
read if you were in a standard atmosphere at your current actual altitude?”
This altitude is called PRESSURE ALTITUDE.
Pressure Altitude can be determined two ways.
- In the aircraft, adjust your altimeter setting to 29.92 in. Hg (standard
pressure), and read the altitude value shown by the altimeter needles.
Or...
- Apply a correction factor from a Pressure Altitude Correction Table
as shown below.
|
In. Hg
|
Conv. Factor
|
In. Hg
|
Conf. Factor
|
In. Hg
|
Conv. Factor
|
In. Hg
|
Conv. Factor
|
|
28.0
|
1824
|
28.8
|
1053
|
29.6
|
298
|
30.3
|
-348
|
|
28.1
|
1727
|
28.9
|
975
|
29.7
|
205
|
30.4
|
-440
|
|
28.2
|
1630
|
29.0
|
863
|
29.8
|
112
|
30.5
|
-531
|
|
28.3
|
1533
|
29.1
|
768
|
29.9
|
20
|
30.6
|
-622
|
|
28.4
|
1336
|
29.2
|
673
|
29.92
|
0
|
30.7
|
-712
|
|
28.5
|
1340
|
29.3
|
579
|
30.0
|
-73
|
30.8
|
-803
|
|
28.6
|
1148
|
29.4
|
485
|
30.1
|
-175
|
30.9
|
-893
|
|
28.7
|
1148
|
29.5
|
392
|
30.2
|
-257
|
31.0
|
-983
|
PRESSURE ALTITUDE CONVERSION TABLE
EXAMPLE:
Airport Altitude = 2367 ft
Altimeter Setting = 30.40 In. Hg
Conversion Factor= -440 feet (from table )
Pressure Altitude = Airport Altitude + Conversion Factor =2367+(- 440) =
1927
NOTE: If your barometric pressure is not shown in the table (say
a value such as 30.35) you will have to interpolate to get the
correct pressure altitude adjustment.
Step 2. Find Density Altitude
Density Altitude uses Pressure Altitude as a basis, and adds in a correction
factor for nonstandard temperature.
Calculate Density Altitude using:
1. PRESSURE ALTITUDE and
2. Outside Air Temperature (OAT)
· Use E6B Flight Computer (see E6B instruction book)
· Use Density Altitude Chart like the one shown below.
For Example: If you found the Pressure Altitude, doing either of the steps
cited above, to be 4000 feet, and the outside Air Temperature (OAT) is
16° , do the following on the chart to find Density Altitude.
Locate 16° C on bottom scale. Go vertically up to intersect the 4000
foot Pressure Altitude slanted line (blue line). Go left horizontally
(blue line) to read Density Altitude = 5000 feet from the left side scale.
You have now adjusted for the difference from standard temperature by
using the chart.
The red line on the chart is a Standard Atmosphere Temperature line.
Performance charts provided by the manufacturer are based on Standard Atmosphere.
Therefore you must adjust your current situation (barometric pressure and
temperature) to Standard Atmosphere. This is done by calculating your Density
Altitude, then using this Density Altitude as the altitude in the manufacturers
performance table when interpreting the performance table data.
Aircraft Performance Charts
Aircraft Performance Charts state performance figures in standard atmosphere
conditions.
Takeoff Performance
You should consult the manufacturers Pilot Operating Handbook for the aircraft
to be flown for takeoff performance tables or graphs.
Takeoff performance is influenced by several factors.
· Adverse conditions
1. High density altitude (high altitude runway, low pressure, high temperature)
2. Runway conditions - mud, soft field, slush, snow, tall grass, rough surface,
uphill
3. Tailwind (downwind takeoff)
4. High gross weight or overload
5. High Humidity
· Favorable conditions
6. Low density altitude (low altitude runway, low temperature, high pressure)
7. Downhill runway
8. Headwind
9. Low weight
10. Low Humidity
Takeoff performance data shown in the manufacturers' charts indicates
the minimum runway requirements necessary for successful
takeoff. Any factor that adversely affects the takeoff distance must be
taken into account to insure safe operation. Consider that the listed
minimum distance is for standard atmospheric conditions, ideal runway
and wind conditions.
|
0000' & 59 deg F |
2500' & 50 deg F |
5000' & 41 deg F |
7500' & 32 deg F |
| GROSS WT. POUNDS |
IAS@50' MPH |
HEAD WIND |
GRND RUN |
CLEAR 50' OBS |
GRND RUN |
CLEAR 50' OBS |
GRND RUN |
CLEAR 50' OBS |
GRND RUN |
CLEAR 50' OBS |
| 2300 |
68 |
0 |
865 |
1525 |
1040 |
1910 |
1255 |
2480 |
1565 |
3855 |
| 2300 |
68 |
10 |
615 |
1170 |
750 |
1485 |
920 |
1955 |
1160 |
3110 |
| 2300 |
68 |
20 |
405 |
850 |
505 |
1100 |
630 |
1480 |
810 |
2425 |
| 2000 |
63 |
0 |
630 |
1095 |
735 |
1325 |
905 |
1625 |
1120 |
2155 |
| 2000 |
63 |
10 |
435 |
820 |
530 |
1005 |
645 |
1250 |
810 |
1685 |
| 2000 |
63 |
20 |
275 |
580 |
340 |
730 |
425 |
910 |
595 |
1255 |
| 1700 |
58 |
0 |
435 |
780 |
520 |
920 |
625 |
1095 |
765 |
1370 |
| 1700 |
58 |
10 |
290 |
570 |
355 |
680 |
430 |
820 |
535 |
1040 |
| 1700 |
58 |
20 |
175 |
385 |
215 |
470 |
270 |
575 |
345 |
745 |
TAKEOFF PERFORMANCE
Wind direction and velocity significantly affect takeoff distance. A
direct headwind will greatest provide takeoff assist. A 90° crosswind
will give no assistance in takeoff. A tailwind component significantly
increases the takeoff roll.
Gross weight affects takeoff performance.
Increased gross weight:
· Requires a higher takeoff speed in order to achieve sufficient lift.
· Results in reduced acceleration due to greater inertia.
· Increases rolling friction , further reducing acceleration.
Gusting or strong crosswinds require that the aircraft be held on the ground
until definite liftoff can be achieved. Once liftoff has occurred, sufficient
speed is needed to prevent settling back onto the runway. If the landing
gear contacts the runway when in a sideways drift, undue stress is placed
on the landing gear.
Glide Performance
Glide performance is the distance that the aircraft will glide with an
inoperative engine. The best distance is attained by gilding at an angle
of attack that provides the maximum lift/drag ratio (L/Dmax).
In the event that the engine becomes inoperative, it is important to
establish the maximum glide airspeed as quickly as possible. This will
permit the maximum radius of emergency landing options. While gliding
toward a suitable landing area, effort should be made to identify the
cause of the failure. If time permits, an engine restart should be attempted
as shown in the start-up check list.
Climb Performance
The Pilot Operating Handbook will contain a Climb Performance chart or
Table similar to the one below for a given aircraft. Note that 4 different
tables are provided. (Sea Level, 5000 ft, 10,000 ft and 15,000 ft). Note
that these altitudes are PRESSURE ALTITUDES and the respective temperatures
are Standard Temperatures for those altitudes. In other words, the values
are given for standard Density Altitudes.
|
Sea Level & 59° F |
5000' & 41° F |
10,000' & 23° |
15,000 & 5° F |
| Gross Weight lbs. |
Ind. Airspeed mph |
Rate of climb ft/min |
Fuel Used gal. |
Ind. Airspeed mph |
Rate of Climb ft/min |
Fuel Used gal |
Ind. Airspeed Ft/min |
Rate of Climb ft/min |
Fuel Used gal. |
Ind. Airspeed mph |
Rate of Climb ft/min |
Fuel Used gal |
| 2300 |
82 |
645 |
1.0 |
81 |
435 |
2.6 |
79 |
230 |
4.8 |
78 |
22 |
11.5 |
| 2000 |
79 |
840 |
1.0 |
79 |
610 |
2.2 |
76 |
380 |
3.6 |
75 |
155 |
6.3 |
| 1700 |
77 |
1085 |
1.0 |
76 |
825 |
1.9 |
73 |
570 |
2.9 |
72 |
315 |
4.4 |
MAXIMUM RATE OF CLIMB DATA
NOTES:
1. Flaps up, full throttle, mixture leaned above 3000 feet for smooth operation.
2. Fuel Used includes, warm-up and takeoff allowance.
3. For hot weather, decrease rate of climb 20 ft/min for each 10°F above
standard day for the particular altitude.
Example:
Given: Gross weight 2000 lb: Pressure Alt. 5000 ft: Temperature 61° F.
SOLUTION:
The rate of climb is 610 at 5000 feet pressure altitude and standard
temperature of 41° F. Since the temperature is 20° F higher that the standard
41°, subtract 40 feet per minute from the 610, to get a rate of climb
= 610 - 40 = 570 ft/min.
Climb performance depends on the aircraft’s reserve power or thrust.
Reserve power is the available power above that required to maintain level
flight at a given airspeed. If an aircraft requires only 120 horsepower
for a given cruise, and the engine is capable of delivering 180 hp., then
the reserve horsepower available for climb is 60 hp.
Two airspeeds are important to the climb performance. These are:
- Vx Best Angle of Climb
- Vy Best Rate of Climb
These V-speeds are defined in the POH. The Best Angle of Climb produces
the greatest altitude in a given distance. The principal use of Best Angle
of Climb is for clearing obstacles on takeoff The Best Rate of Climb produces
the greatest altitude over a given period of time. It is predominately
used as climb to cruise altitude.
Many of the same factors that affect takeoff and cruise performance also
affect climb performance.
Adverse effects:
· Higher than Standard Temperature
· High Humidity
· Lower than Standard Pressure
· Heavy Weight
Heavy weight requires a higher angle of attack to develop adequate lift.
The increased drag results in poorer climb performance. It takes longer
to attain cruise altitude and requires the engine to develop full power
for a longer period of time.
Consult the POH for Climb Performance data for the aircraft to be flown.
Cruise Performance
The cruise performance can be specified two ways.
· Maximum Range
· Maximum Endurance
Maximum Range is the distance that an aircraft can fly
at a given power setting. It requires maximum speed versus fuel flow.
Maximum Duration is the maximum time the aircraft can fly.
This requires that the flight condition must provide for a minimum of
fuel flow.
| ALTITUDE |
RPM |
% PWR |
TAS MPH |
GAL/HR |
END HRS |
RANGE MI. |
| 2500 |
2600 |
81 |
136 |
9.3 |
3.9 |
524 |
| 2500 |
2500 |
73 |
129 |
8.3 |
4.3 |
555 |
| 2500 |
2400 |
65 |
122 |
7.5 |
4.8 |
586 |
| 2500 |
2300 |
56 |
115 |
6.6 |
5.4 |
617 |
| 2500 |
2200 |
52 |
108 |
6.0 |
6.0 |
645 |
| 4500 |
2600 |
77 |
135 |
8.8 |
4.0 |
539 |
| 4500 |
2500 |
69 |
129 |
7.9 |
4.5 |
572 |
| 4500 |
2400 |
62 |
121 |
7.1 |
5.0 |
601 |
| 4500 |
2300 |
56 |
113 |
6.4 |
5.5 |
628 |
| 4500 |
2200 |
51 |
106 |
5.7 |
6.1 |
646 |
| 6500 |
2700 |
81 |
140 |
9.3 |
3.8 |
530 |
| 6500 |
2600 |
73 |
134 |
8.3 |
4.2 |
559 |
| 6500 |
2500 |
66 |
126 |
7.5 |
4.7 |
587 |
| 6500 |
2400 |
60 |
119 |
6.8 |
5.2 |
611 |
| 6500 |
2300 |
54 |
112 |
6.1 |
5.7 |
632 |
| 8500 |
2700 |
77 |
139 |
8.8 |
4.0 |
547 |
| 8500 |
2600 |
70 |
132 |
7.9 |
4.4 |
575 |
| 8500 |
2500 |
63 |
125 |
7.2 |
4.9 |
599 |
| 8500 |
2400 |
57 |
118 |
6.5 |
5.3 |
620 |
| 8500 |
2300 |
52 |
109 |
5.9 |
5.8 |
635 |
| 10500 |
2700 |
73 |
138 |
8.3 |
4.2 |
569 |
| 10500 |
2600 |
66 |
130 |
7.6 |
4.6 |
590 |
| 10500 |
2500 |
60 |
122 |
6.9 |
5.0 |
610 |
| 10500 |
2400 |
55 |
115 |
6.3 |
5.4 |
625 |
| 10500 |
2300 |
50 |
106 |
5.7 |
5.9 |
631 |
CRUISE AND RANGE PERFORMANCE
Crosswind Performance
Takeoffs and landings under significant cross wind conditions can be
dangerous and should be avoided. Crosswinds can be so strong that the
sideways drift cannot be sufficiently overcome by using a “side slip”
into the wind to compensate for the wind drift. Excessive side load on
the landing gear can cause gear failure or an upset aircraft.
The Maximum Crosswind Component for the aircraft will be listed in the
POH. The maximum crosswind is usually about 20% of the landing configuration
stall speed. The diagram above can be used to calculate the headwind and
crosswind components. For most light aircraft, the maximum tested crosswind
component is in the 12 to 15 knot range. In the chart, the numbers around
the periphery of the chart mark the degrees difference between the wind
and the runway heading (magenta lines). The radial lines are are in 5°
increments with numbers on each 10° line.
For example, with a wind of 150° at 30 kt and landing on runway 12 (120°),
the degrees of crosswind will be 150° - 120° = 30°. Locate the 30° radial
line out from the lower left of the graph. This is the differential between
the wind direction and the runway heading. Follow the 30° radial line
(magenta) to the 30kt wind arc (blue). A vertical line (blue) from this
intersection will be the crosswind component of 15 kts. This is the same
as if you had a wind of 15 kts directly from the side.
If you plot a horizontal (blue) line, you will see that your headwind
component is 26 kts. This is the same effect as if you had a direct headwind
of 26 kts.
Landing Performance
The minimum landing distance is attained by landing at the minimum safe
speed which allows sufficient margin above the stall speed for satisfactory
control and go-around capability. Gross weight and headwind are important
considerations in determining minimum landing distance.
Excessive airspeed above that recommended in the POH will significantly
increase landing distance. High density altitude increases landing distance.
As a rule of thumb, the increase in landing distance is about 3.5% for
each 1,000 feet in density altitude.
Braking
A number of factors affect braking. A wet, icy or snow covered runway
will appreciably decrease braking ability. In crosswinds or gusty conditions,
higher than normal approach speed will improve controllability, but will
require longer rollout to stop. A down-sloping runway also increases stopping
distance.
Braking immediately after touchdown is ineffective because the wings
are still producing lift. The pilot should use the natural aerodynamic
drag as much as possible to slow the aircraft. Maintain up-elevator to
a high angle of attack as long as possible. The nose of the aircraft will
settle naturally as airspeed is dissipated. Therefore it is not necessary
(and is unwise) to force the nosewheel hard onto the runway.
After touchdown, hold up-elevators during braking to reduce the load
on the nosewheel. Avoid severe braking to minimize stress on the nose
gear and scrubbing of rubber from the main gear tires.
Gross weight affects stopping ability. Heavy loads and high touchdown
speeds result in greater forward momentum, and require significantly more
runway than normal. The most critical conditions for landing performance
result from some combination of high gross weight , high density altitude
and unfavorable wind conditions. These conditions produce the greatest
landing distance and require the greatest dissipation of energy by the
brakes.
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