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Aerodynamic
Principles of Large-Airplane Upsets To our readers: Loss of airplane control in flight is a leading cause of fatalities in the commercial aviation industry. A variety of reasons exist for airplane upsets, but none is statistically significant. Reducing the number of reasons for upsets is a continual training process, and eliminating one reason will not necessarily reduce the number of loss-of-control accidents and fatalities. Additionally, many reasons for upsets are associated with the environment, in which case avoidance is the best solution, but is not always possible. Therefore, pilots must have the necessary knowledge and skills to recover an upset airplane. Aerodynamic principles of large, swept-wing commercial jet airplanes are similar among all manufacturers. In the interest of safety, and the desire to acknowledge the commonality in recovery techniques, this article was written jointly by Airbus, Boeing Commercial Airplane Group, and Douglas Products Division. The article focuses on Airbus and Boeing airplanes that do not have electronic flight controls, commonly known as fly-by-wire. However, when a fly-by-wire airplane is in a degraded control law (mode), the recovery techniques are appropriate. Additionally, certain conditions can upset any airplane and the basic principles of recognition and recovery still apply regardless of the flight control architecture. Pilots can be exposed to an infinite number of slightly different situations. For this reason, it is not possible to develop specific recovery procedures for each. Operators should address procedural application of techniques within their fleet structures. Pilots who are knowledgeable about aerodynamics and who possess the skills to apply basic recovery techniques can return an upset airplane to normal flight parameters. Airbus and Boeing are dedicating many resources and actively working with an industry team to develop an airplane upset recovery training aid. When it is completed we will make it available to our customers at no charge. Airline flight crews constantly strive to provide passengers with a smooth ride while ensuring an extremely high degree of safety. Pilots in line operation seldom experience the excessive pitch or bank angles associated with an airplane upset. However, with a greater understanding of the fundamental principles of aerodynamics, pilots will be better equipped to successfully maneuver the airplane back to straight-and-level flight in the unlikely event they experience an airplane upset.
Aerodynamic principles applied
to large, swept-wing commercial jet airplanes are similar among all
manufacturers, and the recommended techniques for recovering from an
upset in an airplane subject to these principles are also compatible.
Pilots who understand the conditions of an upset, though such an event
is unlikely, will be better prepared to recover from it. The four conditions
that generally describe an airplane upset (figure 1)
are unintentional:
However, when an airplane is taken to the edges of the flight envelope,
different situations result. It is possible, for example, to encounter
flight conditions where an increase in thrust is needed to maintain
a slower airspeed, and where an increase in pitch will decrease altitude.
While airline pilots may have received training on how to use flight
controls to recover from airplane upsets, they rarely, if ever, experience
these conditions in line operations.
In the context of aerodynamics, the following three basic concepts
should be understood:
The airplane is continuously expending energy in flight because of
drag. Drag is usually offset by using some of the stored chemical
energy -- that is, by burning fuel in the engines. (At landing, the
reverse is the case when wheel brakes [friction] and thrust reversers
dissipate energy.)
During maneuvering, the three types of energy can be traded, or exchanged,
usually at the cost of additional drag. This process of consciously
manipulating the energy state of the airplane is referred to as energy
management. Airspeed (kinetic energy) can be traded for altitude (potential
energy). Altitude therefore can be traded for airspeed, as in a dive.
This trading of energy, however, must be balanced with the final desired
energy state in mind. For example, when a pilot trades altitude for
airspeed by descending the airplane, the descent angle must be selected
carefully in order to capture the final desired energy state with
the introduction of the necessary chemical energy.
This becomes especially important when the pilot wants to generate
aerodynamic forces and moments to maneuver the airplane. Kinetic energy
can be traded for potential energy (climb). Potential energy can be
converted to kinetic energy. Chemical energy can be converted by engines
to either potential or kinetic energy, but only at specified rates.
These relationships are shown in figure 2.
The objective of maneuvering the airplane is to manage energy so
that kinetic energy stays between limits (stall and placards), potential
energy stays within limits (terrain-to-buffet altitude), and chemical
energy stays above certain thresholds (fuel in tanks). These concepts
are especially important to understanding recovery from an airplane
upset.
In managing these energy states and trading between the sources of
energy, the pilot does not directly control the energy. The pilot
controls the direction and magnitude of the forces acting on the airplane.
These forces result in accelerations applied to the airplane. The
result of these accelerations is a change in the orientation of the
airplane and a change in the direction, magnitude, or both, of the
flight path vector. Ultimately, velocity and altitude define the energy
state.
This process of controlling forces to change accelerations and produce
a new energy state takes time. The amount of time required is a function
of the mass of the airplane and the magnitude of the applied forces,
and is governed by Newton's laws. Airplanes of larger mass generally
take longer to change orientation than do smaller ones. This longer
time requires the pilot to plan ahead in a large-mass airplane to
ensure that the actions taken will result in the final desired energy
state.
Thrust, weight, lift, and drag are the forces that act upon an airplane
(figure 3). Maneuvering is accomplished by variations
of these forces and is controlled by the throttles and flight controls.
The lift force in pounds or kilograms generated by a surface is a
result of the angle of attack, the dynamic pressure of the air moving
around it (which is a function of the airspeed and density), and the
size and shape of the surface. Lift varies with angle of attack for
constant speed and air density. As angle of attack is increased, the
lift increases proportionally, and this increase in lift is normally
linear. At a specific angle of attack, however, the resulting lift
due to angle of attack behaves differently. Instead of increasing,
it decreases. At this critical angle of attack, the air moving over
the upper wing surface can no longer remain attached to the surface,
the flow breaks down, and the surface is considered stalled. The breakdown
of the flow and consequent loss of lift is dependent only upon the
angle of attack of the surface. This is true regardless of airplane
speed or attitude. An airplane stall is characterized by any one (or
a combination) of the following conditions:
Flight controls give the pilot the ability to manage the forces acting
on the airplane in order to maneuver; that is, to change the flight
path of the airplane (figure 4).
PITCH CONTROL. An important concept for pilots to understand is that if the airplane
is at a balanced, "in-trim" angle of attack in flight, it
will generally seek to return to the trimmed angle of attack if upset
by external forces or momentary pilot input. This is due to the longitudinal
stability designed into that airplane.
Changes in airplane configuration also affect pitch control. For
example, flap extension usually creates a nose-down pitching moment;
flap retraction usually creates a nose-up pitch. When extended, wing-mounted
speed brakes usually produce a nose-up pitching moment.
Pitch attitude can also change with thrust (figure
5). With underwing engines, reducing thrust creates a nose-down
pitching moment; increasing thrust creates a nose-up pitching moment.
The combination of elevator and stabilizer positions also affects
pitch. In normal maneuvering, the pilot displaces the elevator by
applying an elevator control force. The pilot then trims the stabilizer
by driving it to a new position to remove the elevator control force.
This new stabilizer position is faired with the elevator. If they
are not faired (one is down and the other is up), one cancels out
the other. This condition limits the airplane's ability to overcome
other pitching moments from configuration changes or thrust.
LATERAL AND DIRECTIONAL CONTROL. Motion about the longitudinal axis is called roll (figure
5). Control inputs cause the ailerons and spoilers to control
the airplane's roll rate. The aileron and spoiler movement changes
the local angle of attack of the wing, changing the amount of lift
and causing rotation about the longitudinal axis.
During an airplane upset, unusually large amounts of aileron or spoiler
input may be required to recover the airplane. After input of full
roll control, it may be necessary to use rudder in the direction of
the desired roll. The amount of rudder required to coordinate the
maneuver will depend on the airplane type and associated systems.
An uncoordinated rudder movement results in a nose movement (yaw)
in the direction of the rudder input. The yaw creates sideslip, which
causes a roll in the same direction as the rudder input. The roll
due to sideslip is referred to as dihedral effect.
When encountering an angle of attack associated with the onset of
stick shaker, ailerons and spoilers are still effective at controlling
roll. However, as the angle of attack continues to increase beyond
the angle associated with stick shaker onset, the airflow over the
wing separates and airplane buffet generally begins. Without decreasing
the angle of attack, the combination of ailerons and spoilers in this
separated airflow may not always generate a significant force; therefore,
little rotation about the longitudinal axis occurs on some models.
Since the vertical stabilizer/rudder is rarely aerodynamically stalled,
it is still possible to generate a force and a nose rotation with
associated roll rate.
However, at a high angle of attack, pilots must be extremely careful
when using the rudder for assisting lateral control. Excessive rudder
can cause excessive sideslip which could lead to departure from controlled
flight.
Asymmetric thrust creates a yawing and a rolling moment. An engine
failure creates an undesired yaw and roll. Conversely, an intentional
engine throttle up or down could create a desired yawing moment followed
by a desired rolling moment. Using asymmetric thrust to control roll
is not precise because of the lag time associated with engine spool-up
or spool-down and should be avoided unless no other means of roll
control are available. Generally, the pilot should attempt to restore
symmetric thrust conditions during an upset recovery.
Applying Aerodynamic Fundamentals to Airplane Upsets NOSE HIGH, WINGS LEVEL. In this situation the pilot should trade the potential energy of
altitude for airspeed, and would have to maneuver the airplane's flight
path back toward the horizon. This is accomplished by the input of
up to full nose-down elevator and the use of some nose-down stabilizer
trim. These actions should provide sufficient elevator control power
to produce a nose-down pitch rate. It may be difficult to know how
much stabilizer trim to use, and care must be taken to avoid using
too much trim. Pilots should not fly the airplane using stabilizer
trim, and should stop trimming nose down when they feel the g force
on the airplane lessen or the required elevator force lessen. This
use of stabilizer trim may correct an out-of-trim airplane and solve
a less-critical problem before the pilot must apply further recovery
measures. Because a large nose-down pitch rate will result in a condition
of less than 1 g, at this point the pitch rate should be controlled
by modifying control inputs to maintain between 0 to 1 g. If altitude
permits, flight tests have determined that an effective way to achieve
a nose-down pitch rate is to reduce some thrust on airplanes with
underwing-mounted engines. The use of this technique is not intuitive
and must be considered by each operator for their specific fleet types.
If normal pitch control inputs do not stop an increasing pitch rate,
rolling the airplane to a bank angle that starts the nose down should
work. Bank angles of about 45 degrees, up to a maximum of 60 degrees,
could be needed. Unloading the wing by maintaining continuous nose-down
elevator pressure will keep the wing angle of attack as low as possible,
making the normal roll controls as effective as possible. With airspeed
as low as stick shaker onset, normal roll controls -- up to full deflection
of ailerons and spoilers -- may be used. The rolling maneuver changes
the pitch rate into a turning maneuver, allowing the pitch to decrease.
Finally, if normal pitch control then roll control is ineffective,
careful rudder input in the direction of the desired roll may be required
to induce a rolling maneuver for recovery.
Only a small amount of rudder is needed. Too much rudder applied
too quickly or held too long may result in loss of lateral and directional
control. Because of the low energy condition, pilots should exercise
caution when applying rudder.
The reduced pitch attitude will allow airspeed to increase, thereby
improving elevator and aileron control effectiveness. After the pitch
attitude and airspeed return to a desired range the pilot can reduce
angle of bank with normal lateral flight controls and return the airplane
to normal flight.
NOSE LOW, WINGS LEVEL. Again, it is necessary to maneuver the airplane's flight path back
toward the horizon. At moderate pitch attitudes, applying nose-up
elevator -- and reducing thrust and extending speed brakes, if necessary
-- will change the pitch attitude to a desired range. At extremely
low pitch attitudes and high airspeeds (well above VMO/MMO),
nose-up elevator and nose-up trim may be required to establish a nose-up
pitch rate.
HIGH BANK ANGLES. Any time the airplane is not in "zero-angle-of-bank" flight,
lift created by the wings is not being fully applied against gravity,
and more than 1 g will be required for level flight (figure
6). At bank angles greater than 67 degrees, level flight cannot
be maintained within flight manual limits for a 2.5 g load factor
(figure 7). In high bank angle increasing airspeed
situations, the primary objective is to maneuver the lift of the airplane
to directly oppose the force of gravity by rolling to wings level.
Applying nose-up elevator at bank angles above 60 degrees causes no
appreciable change in pitch attitude and may exceed normal structure
load limits as well as the wing angle of attack for stall. The closer
the lift vector is to vertical (wings level), the more effective the
applied g is in recovering the airplane.
A smooth application of up to full lateral control should provide
enough roll control power to establish a very positive recovery roll
rate. If full roll control application is not satisfactory, it may
even be necessary to apply some rudder in the direction of the desired
roll.
Only a small amount of rudder is needed. Too much rudder applied
too quickly or held too long may result in loss of lateral and directional
control or structural failure.
NOSE HIGH, HIGH BANK ANGLES. NOSE LOW, HIGH BANK ANGLES. Recovery Techniques NOSE-HIGH RECOVERY NOSE-LOW RECOVERY Summary 1. A management overview that identifies the safety concern and encourages
operators to establish an upset recovery training program.
2. A pilot guide that briefly reviews the causes of airplane upsets,
fundamental aerodynamics of flight for large, swept-wing airplanes,
and the application of techniques for recovering an airplane that
has been upset. The guide is a highly readable, concise treatment
for pilot issues written by pilots for pilots. It is intended for
self-study or classroom use.
3. The example airplane upset training program, a stand-alone resource
designed to serve the needs of a training department. An example academic
and simulator training program are both included. The academic program
provides the pilots with the requisite knowledge, and the simulator
training scenarios are designed to help pilots improve their skills
in recovering from an upset.
4. References for additional reading on subjects associated with
airplane upsets and recovery.
Airbus and Boeing encourage all operators to endorse the training
recommendations and include airplane upset recovery training in their
overall pilot training programs.
Dave Carbaugh John Cashman Mike Carriker Doug Forsythe Tom Melody Larry Rockliff William Wainwright return
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The Effect of High
Altitude and Center of Gravity In addition to being fast, quiet, and comfortable, modern commercial airplanes are also aerodynamically efficient. For example, all Boeing transport models use wing sweep to minimize high-speed cruise drag. This allows airplanes to cruise at higher Mach numbers before reaching the critical Mach number at which shock waves begin to form on the wing and drag rises significantly. With the introduction of computers into airplane flight control design, other aerodynamic improvements are possible. However, because these improvements may affect airplane stability, flight crews should be aware of how CG and altitude affect the performance and handling characteristics of the airplanes they fly. This requires an understanding of the following key concepts: 1. Positive and relaxed longitudinal static stability. 1 Positive and Relaxed Longitudinal Static Stability Since download on the tail is negative lift, effectively increasing the weight of the airplane, the location of the CG affects the cruise performance of any airplane. Flying at an aft CG will reduce the download on the tail and improve cruise performance. When airplanes are operated near the aft CG limit, download on the tail is minimized and angles of attack and drag are reduced. However, moving the CG aft reduces the longitudinal static stability of the airplane, something that all flight crews should be aware of (see figure 1 and "Static Longitudinal Stability and Speed Stability" below). As airspeed varies from a trimmed condition, the column force required to maintain a new speed (without re-trimming) is a measure of static longitudinal stability. For any conventional airplane, the location of the CG has the strongest influence on static longitudinal stability. For a statically stable airplane the required column force, as speed varies from the trimmed condition, is less at an aft CG than it is at a forward CG. The minimum average gradient allowed by U.S. Federal Aviation Administration FAR Part 25 is one pound for each six knots. As the CG moves aft, it reaches a point where the stick force per knot drops to zero, then reverses. This location is called the neutral point. The difference between the actual CG location and the neutral point is called the static margin. With a CG forward of the neutral point, an airplane has a positive static margin and positive static longitudinal stability. At a CG aft of the neutral point, an airplane has a negative static margin, is statically unstable, and requires some form of augmentation to be flown with an acceptable workload. 2 Flight Control Computers and Stability Augmentation Augmented stability provides better cruise performance with no increase in workload and no adverse effects from flying at an aft CG. This technology also allows for a smaller tail size, which further reduces drag and weight. However, FAR Part 25 requires that handling qualities remain adequate for continued safe flight and landing following an augmentation system failure. Therefore, a practical limit exists for how far aft the CG can go. The Boeing 777 uses redundant digital flight control computers to provide positive (static longitudinal) stability and enhances that stability with airspeed feedback. The MD-11 uses computers to provide neutral speed stability. In other words, the CG of the MD-11 appears to be at the neutral point. The MD-11 uses elevator deflection to hold attitude at any speed within the normal flight envelope, then trims the stabilizer. This is known as an "attitude hold" system. 3 Maneuvering Stability For example, for the same control surface movement at constant airspeed, an airplane at 35,000 ft (10,670 m) experiences a higher pitch rate than an airplane at 5,000 ft (1,524 m) because there is less aerodynamic damping. The pitch rate is higher, but the resulting change in flight path is not. Therefore, the change in angle of attack is greater, creating more lift and more g. If the control system is designed to provide a fixed ratio of control column force to elevator deflection, it will take less column force to generate the same g as altitude increases. This principle is the essence of high-altitude handling characteristics for RSS airplanes. Unless an RSS airplane has an augmentation system to compensate its maneuvering stability, lighter column forces are required for maneuvering at altitude. Longitudinal maneuvering requires a pitch rate, and the atmosphere provides pitch rate damping. As air density decreases, the pitch rate damping decreases, resulting in decreased maneuvering stability (see figure 2 and "Maneuvering Stability" below). An additional effect is that for a given attitude change, the change in rate of climb is proportional to the true airspeed. Thus, for an attitude change for 500 ft per minute (fpm) at 290 knots indicated air speed (kias) at sea level, the same change in attitude at 290 kias (490 knots true air speed) at 35,000 ft would be almost 900 fpm. This characteristic is essentially true for small attitude changes, such as the kind used to hold altitude. It is also why smooth and small control inputs are required at high altitude, particularly when disconnecting the autopilot. Summary Figure 1: Figure 1 is a plot of speed stability, which is the manner in which static longitudinal stability is demonstrated in flight. It measures the relationship between airspeed and longitudinal control force. Simply stated, speed stability is a measure of the control force required to hold the airplane at an airspeed other than the trimmed airspeed, with the throttles fixed at the trimmed thrust setting. Airplanes with positive static longitudinal stability require a pull force to maintain a speed below the trimmed speed, and a push force to maintain a speed above the trimmed speed. For conventional airplanes (those without stability augmentation), this is a design requirement of the U.S. Federal Aviation Administration Regulations (FAR) Part 25. However, in an unstable airplane--one with negative static longitudinal stability--if the airplane is in trim and the flight crew applies a pull force, the airplane will initially pitch up and slow down, but the pitch rate will quickly become large enough to require a relaxing of the pull, and eventually a push force, to maintain a constant speed below the initial trim speed. The converse is true when the flight crew attempts to accelerate the airplane from the trimmed state. This difficult task can be accomplished without increasing the crew's workload by using electronic flight control computers for stability augmentation. Static Longitudinal Stability and Speed Stability SPEED STABILITY Figure 2: Figure 2 depicts a plot of control column force as it relates to normal acceleration for a stable airplane. It does not represent the data for any specific airplane, but instead reflects the typical maneuvering stability characteristics of a conventional, unaugmented airplane. The left axis displays elevator column force values that increase in the up direction, while the bottom axis displays normal acceleration (g) values that increase in the right direction. The lower the slope, the less the maneuvering stability. The lower-left corner of the graph shows that a certain amount of force must be applied before the airplane starts to move from 1g flight. Called friction and breakout, this situation results from the need to overcome control column static friction and the feel system centering spring. The plot makes it obvious that CG location and its effect on positive longitudinal static stability influence maneuvering stability. The maneuvering stability, or stick force per g, is higher at a forward CG, regardless of altitude. In other words, at any altitude, the stick force perg is higher when the CG is forward than when the CG is further aft. This has significant consequences for steep turning maneuvers. For example, to perform a level turn at 60 degrees of bank requires 2g in any airplane. While the plot shows that the airplane is still more stable at a forward CG than an aft CG, it also shows that altitude greatly affects the force required to pull the same 2g at any CG location. This plot graphically demonstrates that maneuvering at high-altitude requires less column force than it does at low altitude. MANEUVERING STABILITY A column force is required to maneuver longitudinally. For most airplanes, static stability attempts to maintain the airplane in 1g flight at the trimmed angle of attack. The column force generates a pitching moment through the elevators, or stabilizer in some airplanes, that is eventually balanced by the damping moment created by the horizontal tail and the moment due to the change in angle of attack. At this point, if the force is maintained, and there is enough thrust to maintain airspeed, the airplane stabilizes at a new angle of attack, with corresponding changes in lift and g. Since the pitching moments are now balanced, the pilot must hold the column force. If the column force is released, the pitching moment due to the elevator or stabilizer goes to zero, and the moments due to pitch rate and angle of attack drive the pitch rate to zero, and the airplane returns to 1g flight. This description of maneuvering flight points out that maneuvering stability for a given configuration manifests itself to the flight crew as the column force required to maintain a certain level of g. This is commonly called "stick force per g." return
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