5.2 Critical Mach Number, Shock Waves & Compressibility Buffet
Key Takeaways
Critical Mach number (Mcrit) is the freestream Mach at which local airflow somewhere on the aerofoil first reaches Mach 1 — typically on the upper surface near maximum thickness.
A shock wave is an abrupt, nearly discontinuous compression where supersonic flow decelerates to subsonic; normal shocks maximise pressure rise and drag, oblique shocks are weaker and angled to the flow.
Shock-induced boundary-layer separation creates wave drag, buffet, and a rearward shift of centre of pressure that can produce Mach tuck if uncorrected.
Compressibility buffet is an oscillatory separation behind a fluctuating shock on the wing; it warns the aircraft is operating near or beyond the buffet onset boundary.
Higher sweep, thinner sections, and lower cruise lift coefficient all raise Mcrit; supercritical aerofoils delay strong shocks to permit higher cruise Mach.
5.2 Critical Mach Number, Shock Waves & Compressibility Buffet
When a swept-wing jet accelerates toward cruise Mach, the wing does not need to fly at M = 1 for serious compressibility problems to begin. EASA Part-66 Module 08 requires you to understand critical Mach number, how shock waves form, and why compressibility buffet appears — because these set , buffet margins, and Mach trim requirements on modern transports.
Critical Mach Number ()
Critical Mach number () is defined as the freestream Mach number at which the airflow first reaches Mach 1 at some point on the aerofoil surface — almost always on the upper (suction) side where the camber accelerates flow.
Below : entirely subsonic surface flow; shocks absent. At : a sonic point appears (often near max thickness, ~30–40% chord). Above : a supersonic pocket forms on the upper surface, terminated by a shock wave.
| Factor | Effect on |
|---|---|
| Thicker aerofoil section | Lowers (stronger acceleration) |
| Higher angle of attack / | Lowers (more upper-surface suction) |
| Greater wing sweep | Raises (see Section 5.3) |
| Supercritical aerofoil design | Raises effective cruise Mach (weakens shock) |
For a typical 1950s straight-wing section, might be ~0.70. A modern supercritical section on a swept wing may permit cruise at M 0.82–0.86 because the shock is weaker and farther aft.
Shock Waves — Normal and Oblique
A shock wave is a thin region of extremely rapid compression where flow properties change almost discontinuously. Shocks form when supersonic flow must slow to subsonic conditions (e.g., at the downstream end of a supersonic pocket on a wing, or at a pitot intake lip).
Freestream M < 1 Supersonic pocket on upper surface
| ___________
=====|=====> subsonic everywhere / \ supersonic region
| | | \
Wing surface | SHOCK → subsonic wake
Wing surface
Normal shock (M2 ≈ 1) Oblique shock (M2 may remain > 1)
| | /
====>| |==== subsonic /====> turned flow
| | /
perpendicular angled to flow
Normal shock: Shock front perpendicular to flow. Large pressure, density, and temperature rise; velocity drops from supersonic to subsonic in one step. Maximum entropy rise — very high wave drag.
Oblique shock: Inclined at angle to upstream flow. Weaker than a normal shock at the same upstream Mach; downstream flow may remain supersonic (weak oblique shock) or become subsonic (strong oblique shock).
Across any shock:
- Static pressure, temperature, and density increase
- Total pressure decreases (irreversible — energy lost to drag and heating)
- Boundary layer may separate if adverse pressure gradient is severe
Wave Drag, Centre-of-Pressure Shift & Mach Tuck
The pressure jump across a shock adds a component of wave drag — drag unrelated to skin friction or induced drag. As Mach increases past , wave drag rises sharply; the drag divergence Mach is where becomes steep.
Simultaneously, the centre of pressure (CP) on the wing moves aft because suction aft of the shock weakens and the shock-induced pressure rise acts predominantly on the rearward upper surface. This nose-down pitching tendency is called Mach tuck. Transport aircraft employ:
- Mach trim systems (automatic stabiliser or THS input)
- Swept wings and washout
- Limiting in the AFM
If Mach tuck is not trimmed and the aircraft accelerates beyond the approved envelope, dive tendency can intensify — a flight-test and certification concern, not merely academic theory.
Compressibility Buffet
Compressibility buffet (shock buffet) is an aerodynamic oscillation caused by intermittent shock-induced boundary-layer separation on the wing. The shock position moves forward and aft; the separated wake grows and collapses, producing vibrations felt in the fuselage and often registering on g meters.
Characteristics:
- Onset near buffet onset boundary in the flight envelope — often a few hundredths of Mach below
- Worsens at higher altitude (lower Reynolds number, thinner boundary layer)
- Worsens at higher g or angle of attack (higher local suction)
- Distinct from stall buffet (low speed, low Mach, wing-root separation)
Pilots use buffet as a tactile warning; engineers document buffet boundaries during certification. For maintenance, recurring buffet reports at normal cruise may indicate wing contamination (ice, damage, mis-rigged high-lift devices) or AFM exceedance — not something to dismiss as "turbulence."
Worked Example 5.2.1: Identifying from Description
Problem: Flight test notes state: "At M 0.75, schlieren imaging shows entirely subsonic flow. At M 0.78, a local sonic point appears at 38% chord on the upper surface. At M 0.80, a terminated supersonic region and visible shock are present." What is ?
Solution: is the lowest freestream Mach where local M = 1 first appears — here M 0.78. At M 0.80 the shock is fully formed, which is above .
Worked Example 5.2.2: Buffet vs Stall
Problem: A B737 at FL 370 experiences moderate airframe rumble at M 0.82 and 1.25g in light turbulence. IAS is 245 kt; stall speed at this weight is 195 kt IAS. Is compressibility buffet plausible?
Solution: IAS is well above stall speed — stall buffet is unlikely. At FL 370, M 0.82 is near typical for this class; high g increases local and lowers local . Compressibility buffet is plausible — check AFM Mach/g envelope and whether the aircraft is at or above buffet onset.
Exam Traps
- is a freestream value, not the local peak Mach on the surface (which can be > 1 when ).
- Shocks always increase static temperature — aerodynamic heating begins here (Section 5.3).
- Buffet at high altitude/high Mach is not always stall — check Mach and g limits first.
- Wave drag appears only with shocks, not in purely subsonic flow.
- Mach tuck is a CP shift, not engine failure or CG movement — though it affects pitch trim loads on the tailplane.
What is the critical Mach number (Mcrit) of an aerofoil?
The Mach number at which the aircraft's true airspeed equals 340 m/s
The freestream Mach at which local flow somewhere on the aerofoil first reaches Mach 1
The freestream Mach at which lift coefficient reaches maximum
The highest Mach number permitted by the AFM (MMO)
Compared with an oblique shock at the same upstream Mach number, a normal shock produces:
A greater pressure rise and higher wave drag
No change in static temperature
A smaller pressure rise and lower wave drag
Only a reduction in density without pressure change
Compressibility buffet on a swept-wing jet in high-speed cruise is primarily caused by:
Propeller blade tip stall at low rpm
Engine compressor surge due to intake icing
Oscillating shock-induced boundary-layer separation on the wing
Excessive dihedral effect in the landing configuration
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