Mach Number

Introduction to the Mach Number

The Mach Number is a dimensionless value useful for analyzing fluid flow dynamics problems where compressibility is a significant factor.

The Mach Number can be expressed as

M = v / c         (1)


M = Mach number

v = fluid flow speed (m/s, ft/s)

c = speed of sound (m/s, ft/s)

Alternatively the Mach Number can be expressed with the density and the bulk modulus for elasticity as

M = v (ρ / E)1/2         (2)


ρ = density of fluid (kg/m3, lb/ft3)

E = bulk modulus elasticity (N/m2 (Pa), lbf/in2 (psi))

The bulk modulus elasticity has the dimension pressure and is commonly used to characterize the fluid compressibility.

The square of the Mach number is the Cauchy Number.

M2 = C          (3)


C = Cauchy Number

Subsonic and Supersonic speed

  • If the mach number is < 1, the flow speed is lower than the speed of sound - and the speed is subsonic.
  • If the mach number is ~ 1, the flow speed is approximately like the speed of sound - and the speed is transonic.
  • If the mach number is > 1, the flow speed is higher than the speed of sound - and the speed is supersonic.
  • If the mach number is >> 1, the flow speed is much higher than the speed of sound - and the speed is hypersonic.

Example - Calculating an Aircraft Mach Number

An aircraft flies at speed 500 mph at an altitude of 35.000 ft. The surrounding temperature is -60 oF.

The sound speed at this altitude and temperature can be calculated as

c = [k R T]1/2

    = [ 1.4 (1716 ft lb/slug oR) ((-60 oF) + (460 oR)) ]1/2

    = 980 ft/s


k = 1.4

R = 1716 (ft lb/slug oR)

The speed of the aircraft can be calculated as

v = (500 miles/hr) (5280 ft/miles) / (3600 sec/hr)

    = 733 ft/sec

The Mach Number can be calculated as

M = (733 ft/s) / (980 ft/s)

= 0.75 - the aircraft is flying at subsonic speed

Related Topics

  • Fluid Mechanics - The study of fluids - liquids and gases. Involves various properties of the fluid, such as velocity, pressure, density and temperature, as functions of space and time.

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