Wings generate much of their lift due to the Bernoulli effect; by speeding up the airflow over the top of the wing, the air has less density on top than on the bottom, leading to a net upward force. The relative difference in speed is due largely to the wing's shape, so the difference in speed remains a fairly constant ratio over a wide range of speeds.
But if the air speed on the top of the wing is faster than on the bottom, there will be some speed where the air on top reaches the speed of sound. This is the critical mach. When this happens shock waves form on the upper wing at the point where the flow becomes supersonic, typically behind the midline of the chord. Shock waves generate lift of their own, so the lift of the wing suddenly moves rearward, twisting it down. This effect is known as mach tuck.
The actual speed of critical mach varies from wing to wing. In general a thicker wing will have a lower critical mach, because a thicker wing accelerates the airflow more than a thinner one. For instance, the fairly thick wing on the P-38 Lightning led to a critical mach of about .69 Mach, a speed it could reach with some ease in dives, which lead to a number of crashes. The much thinner wing on the Supermarine Spitfire was deliberately chosen to avoid this problem, and had a critical mach of about .89 Mach.
Today a compromise design is used, the swept-wing. This design "fools" the air into thinking it's flowing over a thin wing, which is in fact fairly thick. Swept-wings are used on almost all aircraft that fly in the transonic, and is a common feature of almost all airliners and modern fighter aircraft.
It is possible to see the mach line on an airliner visually, as these aircraft fly beyond the critical mach in crusing flight. The shock wave extends vertically off of the wing, and the change in density is enough to make it operate as a lens. By looking at straight lines running parallel to the wing you can often spot a discontinuity where the line "jumps". Roads are an excellent marker for this.
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