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 $M_{MO}$, buffet margins, and Mach trim requirements on modern transports.
Critical Mach Number ($M_{crit}$)
Critical Mach number ($M_{crit}$) 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 $M_{crit}$: entirely subsonic surface flow; shocks absent. At $M_{crit}$: a sonic point appears (often near max thickness, ~30–40% chord). Above $M_{crit}$: a supersonic pocket forms on the upper surface, terminated by a shock wave.
| Factor | Effect on $M_{crit}$ |
|---|---|
| Thicker aerofoil section | Lowers $M_{crit}$ (stronger acceleration) |
| Higher angle of attack / $C_L$ | Lowers $M_{crit}$ (more upper-surface suction) |
| Greater wing sweep $\Lambda$ | Raises $M_{crit}$ (see Section 5.3) |
| Supercritical aerofoil design | Raises effective cruise Mach (weakens shock) |
For a typical 1950s straight-wing section, $M_{crit}$ 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 $\beta$ 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 $M_{crit}$, wave drag rises sharply; the drag divergence Mach is where $\mathrm{d}C_D/\mathrm{d}M$ 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 $M_{MO}$ 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 $M_{MO}$
- 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 $M_{crit}$ 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 $M_{crit}$?
Solution: $M_{crit}$ 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 $M_{crit}$.
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 $M_{MO}$ for this class; high g increases local $C_L$ and lowers local $M_{crit}$. Compressibility buffet is plausible — check AFM Mach/g envelope and whether the aircraft is at or above buffet onset.
Exam Traps
- $M_{crit}$ is a freestream value, not the local peak Mach on the surface (which can be > 1 when $M_\infty = M_{crit}$).
- 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?
Compared with an oblique shock at the same upstream Mach number, a normal shock produces:
Compressibility buffet on a swept-wing jet in high-speed cruise is primarily caused by: