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PHAK 10.6 Takeoff and Landing Performance

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The majority of pilot-caused aircraft accidents occur during the takeoff and landing phase of flight. Because of this fact, the pilot must be familiar with all the variables that influence the takeoff and landing performance of an aircraft and must strive for exacting, professional procedures of operation during these phases of flight.

Takeoff and landing performance is a condition of accelerated and decelerated motion. For instance, during takeoff, an aircraft starts at zero speed and accelerates to the takeoff speed to become airborne. During landing, the aircraft touches down at the landing speed and decelerates to zero speed. The important factors of takeoff or landing performance are:

  • The takeoff or landing speed is generally a function of the stall speed or minimum flying speed.
  • The rate of acceleration/deceleration during the takeoff or landing roll. The speed experienced by any object varies directly with the imbalance of force and inversely with the mass of the object. An airplane on the runway moving at 75 knots has four times the energy it has traveling at 37 knots. Thus, an airplane requires four times as much distance to stop as required at half the speed.
  • The takeoff or landing roll distance is a function of both acceleration/deceleration and speed.

10.6.1 Runway Surface and Gradient #

Runway conditions affect takeoff and landing performance. Typically, performance chart information assumes paved, level, smooth, and dry runway surfaces. Since no two runways are alike, the runway surface differs from one runway to another, as does the runway gradient or slope. [Figure 10-15]

Figure 10-15. An aircraft performance depends greatly on the runway surface.
Figure 10-15. An aircraft performance depends greatly on the runway surface.

Runway surfaces vary widely from one airport to another. The runway surface encountered may be concrete, asphalt, gravel, dirt, or grass. The runway surface for a specific airport is noted in the Airport/Facility Directory (A/FD). Any surface that is not hard and smooth will increase the ground roll during takeoff. This is due to the inability of the tires to roll smoothly along the runway. Tires can sink into soft, grassy, or muddy runways. Potholes or other ruts in the pavement can be the cause of poor tire movement along the runway. Obstructions such as mud, snow, or standing water reduce the airplane’s acceleration down the runway. Although muddy and wet surface conditions can reduce friction between the runway and the tires, they can also act as obstructions and reduce the landing distance. [Figure 10-16] Braking effectiveness is another consideration when dealing with various runway types. The condition of the surface affects the braking ability of the airplane.

The amount of power that is applied to the brakes without skidding the tires is referred to as braking effectiveness.

Figure 10-16. Airport/facility directory (A/FD) information.
Figure 10-16. Airport/facility directory (A/FD) information.

Ensure that runways are adequate in length for takeoff acceleration and landing deceleration when less than ideal surface conditions are being reported.

The gradient or slope of the runway is the amount of change in runway height over the length of the runway. The gradient is expressed as a percentage such as a 3 percent gradient. This means that for every 100 feet of runway length, the runway height changes by 3 feet. A positive gradient indicates the runway height increases, and a negative gradient indicates the runway decreases in height. An upsloping runway impedes acceleration and results in a longer ground run during takeoff. However, landing on an upsloping runway typically reduces the landing roll. A downsloping runway aids in acceleration on takeoff resulting in shorter takeoff distances. The opposite is true when landing, as landing on a downsloping runway increases landing distances. Runway slope information is contained in the A/FD.

10.6.2 Water on the Runway and Dynamic Hydroplaning #

Water on the runways reduces the friction between the tires and the ground, and can reduce braking effectiveness. The ability to brake can be completely lost when the tires are hydroplaning because a layer of water separates the tires from the runway surface. This is also true of braking effectiveness when runways are covered in ice.

When the runway is wet, the pilot may be confronted with dynamic hydroplaning. Dynamic hydroplaning is a condition in which the aircraft tires ride on a thin sheet of water rather than on the runway’s surface. Because hydroplaning wheels are not touching the runway, braking and directional control are almost nil. To help minimize dynamic hydroplaning, some runways are grooved to help drain off water; most runways are not.

Tire pressure is a factor in dynamic hydroplaning. Using the simple formula in Figure 10-17, a pilot can calculate the minimum speed, in knots, at which hydroplaning will begin. In plain language, the minimum hydroplaning speed is determined by multiplying the square root of the main gear tire pressure in psi by nine. For example, if the main gear tire pressure is at 36 psi, the aircraft would begin hydroplaning at approximately 54 knots.

Figure 10-17. Tire pressure.
Figure 10-17. Tire pressure.

Landing at higher than recommended touchdown speeds will expose the aircraft to a greater potential for hydroplaning. And once hydroplaning starts, it can continue well below the minimum initial hydroplaning speed.

On wet runways, directional control can be maximized by landing into the wind. Abrupt control inputs should be avoided. When the runway is wet, anticipate braking problems well before landing and be prepared for hydroplaning. Opt for a suitable runway most aligned with the wind. Mechanical braking may be ineffective, so aerodynamic braking should be used to its fullest advantage.

10.6.3 Takeoff Performance #

The minimum takeoff distance is of primary interest in the operation of any aircraft because it defines the runway requirements. The minimum takeoff distance is obtained by taking off at some minimum safe speed that allows sufficient margin above stall and provides satisfactory control and initial rate of climb. Generally, the lift-off speed is some fixed percentage of the stall speed or minimum control speed for the aircraft in the takeoff configuration. Depending on the aircraft characteristics, the lift-off speed will be anywhere from 1.05 to 1.25 times the stall speed or minimum control speed.

To obtain minimum takeoff distance at the specific lift-off speed, the forces that act on the aircraft must provide the maximum acceleration during the takeoff roll.

The powerplant thrust is the principal force to provide the acceleration and, for minimum takeoff distance, the output thrust should be at a maximum. Any item that alters the takeoff speed or acceleration rate during the takeoff roll will affect the takeoff distance. Increased gross weight can be considered to produce a threefold effect on takeoff performance: 1. Higher lift-off speed; 2. Greater mass to accelerate; 3. Increased retarding force (drag and ground friction). As an example of the effect of a change in gross weight, a 21 percent increase in takeoff weight will require a 10 percent increase in lift-off speed to support the greater weight. If the aircraft has a relatively high thrust-to-weight ratio, the change in the net accelerating force is slight and the principal effect on acceleration is due to the change in mass.

For example, a 10 percent increase in takeoff gross weight would cause:

  • A 5 percent increase in takeoff velocity.
  • At least a 9 percent decrease in rate of acceleration.
  • At least a 21 percent increase in takeoff distance.

With ISA conditions, increasing the takeoff weight of the average Cessna 182 from 2,400 pounds to 2,700 pounds (11 percent increase) results in an increased takeoff distance from 440 feet to 575 feet (23 percent increase).

The effect of wind on takeoff distance is large. The effect of a headwind is to allow the aircraft to reach the lift-off speed at a lower groundspeed while the effect of a tailwind is to require the aircraft to achieve a greater groundspeed to attain the lift-off speed.

A headwind that is 10 percent of the takeoff airspeed will reduce the takeoff distance approximately 19 percent. However, a tailwind that is 10 percent of the takeoff airspeed will increase the takeoff distance approximately 21 percent. In the case where the headwind speed is 50 percent of the takeoff speed, the takeoff distance would be approximately 25 percent of the zero wind takeoff distance (75 percent reduction).

The effect of wind on landing distance is identical to its effect on takeoff distance. Figure 10-18 illustrates the general effect of wind. The takeoff speeds specified in the AFM/POH are generally the minimum safe speeds at which the aircraft can become airborne. Any attempt to take off below the recommended speed means that the aircraft could stall, be difficult to

Figure 10-18. Effect of wind on takeoff and landing.
Figure 10-18. Effect of wind on takeoff and landing.

control, or have a very low initial rate of climb. On the other hand, an excessive airspeed at takeoff may improve the initial rate of climb and “feel” of the aircraft, but will produce an undesirable increase in takeoff distance. Assuming that the acceleration is essentially unaffected, the takeoff distance varies with the square of the takeoff velocity.

Thus, ten percent excess airspeed would increase the takeoff distance 21 percent.

The effect of pressure altitude and ambient temperature is to define the density altitude and its effect on takeoff performance. An increase in density altitude can produce a twofold effect on takeoff performance: 1. Greater takeoff speed; 2. Decreased thrust and reduced net accelerating force. The aircraft at altitude will take off at the same indicated airspeed (IAS) as at sea level, but because of the reduced air density, the TAS will be greater. An increase in altitude above standard sea level will bring an immediate decrease in power output for the unsupercharged reciprocating engine; for the supercharged reciprocating engine it will not cause a decrease until the altitude exceeds the critical operating altitude. The most critical conditions of takeoff performance are the result of some combination of high gross weight, altitude, temperature, and unfavorable wind. In the prediction of takeoff distance from the AFM/POH data, the following primary considerations must be given:

  • Pressure altitude and temperature—to define the effect of density altitude on distance
  • Gross weight—a large effect on distance
  • Wind—a large effect due to the wind or wind component along the runway
  • Runway slope and condition—the effect of an incline and retarding effect of factors such as snow or ice

10.6.4 Landing Performance #

In many cases, the landing distance of an aircraft will define the runway requirements for flight operations. The minimum landing distance is obtained by landing at some minimum safe speed, which allows sufficient margin above stall and provides satisfactory control and capability for a go-around. Generally, the landing speed is some fixed percentage of the stall speed or minimum control speed for the aircraft in the landing configuration. The exact values will depend on the aircraft characteristics but, once defined, the values are independent of weight, altitude, and wind.

To obtain minimum landing distance at the specified landing speed, the forces that act on the aircraft must provide maximum deceleration during the landing roll. Minimum landing distance will be obtained by creating a continuous peak deceleration of the aircraft; that is, extensive use of the brakes for maximum deceleration. On the other hand, an ordinary landing roll with considerable excess runway may allow extensive use of aerodynamic drag to minimize wear and tear on the tires and brakes. The use of aerodynamic drag is applicable only for deceleration to 60 or 70 percent of the touchdown speed. At speeds less than 60 to 70 percent of the touchdown speed, aerodynamic drag is so slight as to be of little use, and braking must be utilized to produce continued deceleration.

The effect of gross weight on landing distance is one of the principal items determining the landing distance. For an example of the effect of a change in gross weight, a 21 percent increase in landing weight will require a ten percent increase in landing speed to support the greater weight.

When minimum landing distances are considered, braking friction forces predominate during the landing roll, and the minimum landing distance will vary in direct proportion to the gross weight. For example, a ten percent increase in gross weight at landing would cause a:

  • Five percent increase in landing velocity
  • Ten percent increase in landing distance

The effect of wind on landing distance is large. Since the aircraft will land at a particular airspeed independent of the wind, the principal effect of wind on landing distance is the change in the groundspeed at which the aircraft touches down.

The effect of pressure altitude and ambient temperature is to define density altitude and its effect on landing performance. An increase in density altitude increases the landing speed but does not alter the net retarding force. Thus, the aircraft at altitude lands at the same IAS as at sea level but, because of the reduced density, the TAS is greater. Since an increase in altitude does not alter deceleration, the effect of density altitude on landing distance is due to the greater TAS.

The minimum landing distance at 5,000 feet is 16 percent greater than the minimum landing distance at sea level — approximately three and one-half percent for each 1,000 feet of altitude.

A ten percent excess landing speed causes at least a 21 percent increase in landing distance.

The most critical conditions of landing performance are combinations of high gross weight, high density altitude, and unfavorable wind.

In the prediction of minimum landing distance from the AFM/POH data, the following considerations must be given:

  • Pressure altitude and temperature—to define the effect of density altitude
  • Gross weight—which defines the CAS for landing
  • Wind—a large effect due to wind or wind component along the runway
  • Runway slope and condition—relatively small correction for ordinary values of runway slope, but a significant effect of snow, ice, or soft ground

As an illustration of how errors compound: a pilot is downwind for runway 18, and the tower asks if runway 27 could be accepted. There is a light rain and the winds are out of the east at ten knots. The pilot accepts; the turn is tight, and the pilot must dive to reach runway 27. After becoming aligned with the runway and at 50 feet AGL, the pilot is already 1,000 feet down the 3,500 foot runway, with airspeed still high by about ten percent (about 80 knots versus a target 70 knots) and a ten-knot tailwind. The high airspeed alone increases the landing distance by about 20 percent (from a planned 1,600 feet to 1,920 feet). The tailwind adds roughly another 20 percent (about 320 feet), for a total of about 2,240 feet after reaching 50 feet AGL. Added to the 1,000 feet of overshoot, the total required is about 3,240 feet on a 3,500 foot runway — only 260 feet to spare, and that is in a perfect environment. A typical pilot reaction is to brake hard; the brakes lock, and the aircraft hydroplanes on the wet surface until decreasing to about 54 knots (the square root of the tire pressure √36 × 9), during which braking is ineffective. The apparent margin has long since evaporated. Bad decisions, when combined, have a synergy greater than the individual errors. Aeronautical decision-making is discussed more fully in Chapter 17, Aeronautical Decision-Making (ADM).

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