Mach tuck

Mach tuck is an aerodynamic effect, whereby the nose of an aircraft tends to pitch downwards as the airflow around the wing reaches supersonic speeds. The aircraft will be subsonic, and traveling significantly below Mach 1.0, when it first experiences this effect.[1]

Contents

Causes of Mach tuck

Mach tuck is dependent upon the dynamics of lift.

Mach tuck is the result of an aerodynamic stall due to an over-speed condition, rather than the more common stalls resulting from boundary layer separation due to insufficient airspeed, increased angle of attack, excessive load factors, or a combination of those causes. As the aircraft's wing approaches its critical Mach number, the aircraft is traveling below Mach 1.0. However, the accelerated airflow over the upper surface of the cambered wing exceeds Mach 1.0 and a shock wave is created at the point on the wing where the accelerated airflow has gone supersonic. While the air ahead of the shock wave is in laminar flow, a boundary layer separation is created aft of the shock wave, and that section of the wing fails to produce lift. The image to the right illustrates this concept.

In most aircraft susceptible to Mach tuck, the camber at the wing root, the section of the wing closest to the fuselage, is more pronounced than that of the wing tip. This design ensures that in a standard stall the root will stall before the tips. This allows the pilot to recognize the stall while still maintaining control of the ailerons to enhance stall recovery. However, this also means that when an airfoil exceeds its critical Mach number, the shock wave, and resulting stall condition, will begin to form at the root.

A second design element that leads to Mach tuck is that many aircraft which will approach the speed of sound are designed with swept wings. The center of pressure of a wing is an imaginary point where the summation of all lifting forces across the wing's surface can be resolved into a single lift vector. When the wing root stalls, the center of pressure of the (reduced) lift being generated by the wing is shifted towards the wing tip. With a swept wing, this also means that the center of pressure travels aft (because it is traveling out from the wing root and therefore backwards as the wing sweeps). When the center of pressure moves aft, its movement rearwards compared to the unmoving center of mass of the aircraft will generate a force which will act to depress the nose of the aircraft; this nose down pitching moment is “Mach tuck."

As the wing becomes more affected by the shock wave the center of pressure will continue to travel aft, thereby causing a significantly higher nose-down force and requiring a nose-up input or trim to maintain level flight. Although Mach tuck develops gradually, if it is allowed to progress significantly, the center of pressure can move so far rearward that there is no longer enough elevator authority available to counteract it, and the airplane enters a steep, sometimes unrecoverable dive.[2]

In addition, until the aircraft goes supersonic, as the shock wave goes towards the rear, because of the faster flow there the top shockwave will impinge upon the horizontal stabilizer and elevator control surfaces further back than the lower shockwave; this can greatly exacerbate the nose down tendencies. The horizontal stabilizer at the tail of the aircraft generates a downward force, so loss of effective horizontal stabilizer area will reduce this downward force, so the tail will pitch up and the nose will pitch down. If the shock wave affects the elevators, it may reduce their effectiveness, making it impossible for the pilot to alter the aircraft's pitch.[3]

Finally, there is a related condition that can exacerbate Mach tuck. If enough of the wing surface becomes engulfed in the shock wave, the wing will not produce enough lift to support the aircraft, and a standard stall will occur. This often fatal combination of overspeed and aerodynamic stall can most easily be avoided by not allowing the effects of Mach tuck to develop beyond its incipient stage. This is best accomplished by retarding the throttle, extending speed brakes, and if possible, extending the landing gear. Any actions, which would increase aerodynamic drag and thus reduce airspeed below critical Mach, will prevent further aggravation of the condition.

Dealing with Mach tuck

All supersonic aircraft experience some degree of mach tuck.

Historically, recovery from a mach tuck in subsonic aircraft has not always been possible. In some cases, as the aircraft descends, the air density increases and the extra drag will slow the aircraft and control will return.

For aircraft such as supersonic fighters/bombers or supersonic transports such as Concorde that spend long periods in supersonic flight, Mach tuck is often compensated for by moving fuel between tanks in the fuselage to change the position of the centre of mass. This minimizes the amount of trim required and keeps the changing location of the center of pressure within acceptable limits.

Supersonic and subsonic aircraft often have an all-moving tailplane (a stabilator) rather than separate elevator control surfaces. This avoids the shock wave making the control surfaces pitch downwards.[3]

History

World War II fighters with high power engines capable of producing extremely high airspeeds were the first aircraft to experience Mach tuck. Because research with supersonic airfoils was in its infancy, there were no wings with the design elements that aid in slowing the onset of the Mach tuck effects. Instead, the shock wave would engulf the entire wing, making recovery much more difficult.

The P-38 was the first 400 mph fighter and it suffered more than the usual teething troubles. It had a thick, high-lift wing for fast climb characteristics and for holding a large fuel supply. It also had three fuselages: the central weapon and pilot nacelle or gondola, and the twin booms containing engines and turbosuperchargers. Finally, it was a very densely weighted fighter for its day, and accelerated quickly to terminal velocity in a dive. Bernoulli's effect worked very strongly on the thick wing, and was even more pronounced where air was pushed out of the way by and compressed between the central nacelle and the engine booms. Mach tuck would occur when the aircraft attained Mach 0.68 at which point the air flow over the wing roots would go transonic. The wing would lose lift and the normal loading of the tail's horizontal control surfaces would move aft, leaving the elevator unloaded, bringing the nose further down in a Mach tuck. Lockheed engineers eventually found a solution whereby a small 'speed bump' flap on the underside of the wing would be engaged by a pilot initiating a dive. The flap changed the center of pressure distribution so that the wing would not lose its lift.[4]

References

  1. ^ Pilot’s Handbook of Aeronautical Knowledge. U.S. Government Printing Office, Washington D.C.: U.S. Federal Aviation Administration. 2003. pp. 3–37 to 3–38. FAA-8083-25. http://www.faa.gov/library/manuals/aviation/pilot_handbook/. 
  2. ^ Airplane Flying Handbook. U.S. Government Printing Office, Washington D.C.: U.S. Federal Aviation Administration. 2004. pp. 15–7 to 15–8. FAA-8083-3A. http://www.faa.gov/library/manuals/aircraft/airplane_handbook/. 
  3. ^ a b Transonic Aircraft Design
  4. ^ Bodie, Warren M. The Lockheed P-38 Lightning: The Definitive Story of Lockheed's P-38 Fighter. Hayesville, North Carolina: Widewing Publications, 2001, 1991. ISBN 0-96293-595-6.

 This article incorporates public domain material from the United States Government document "Airplane Flying Handbook".
 This article incorporates public domain material from the United States Government document "Pilot's Handbook of Aeronautical Knowledge".