Speed of Sound Equations
Calculate the speed of sound (the sonic velocity) in gases, fluids or solids.
A disturbance introduced in some point of a substance  solid or fluid  will propagate through the substance as a wave with a finite velocity.
Acoustic Velocity and Speed of Sound
The velocity at which a small disturbance will propagate through the medium is called Acoustic Velocity or Speed of Sound.
Note that speed is a scalar quantity. Velocity is vector quantity with direction.
The acoustic velocity is related to the change in pressure and density of the substance and can be expressed as
c = (dp / dρ)^{1/2} (1)
where
c = speed of sound (m/s, ft/s)
dp = change in pressure (Pa, psi)
dρ = change in density (kg/m^{3}, lb/ft^{3})
Speed of Sound in Gases, Fluids and Solids
The acoustic velocity can alternatively be expressed with Hook's Law as
c = (K / ρ)^{1/2} (2)
where
K = Bulk Modulus of Elasticity (Pa, psi)
ρ = density (kg/m^{3}, lb/ft^{3})
This equation is valid for liquids, solids and gases. The sound travels faster through media with higher elasticity and/or lower density. If a medium is not compressible at all  incompressible  the speed of sound is infinite (c ≈ ∞).
Substance  Bulk Modulus Elasticity  K  (10^{9} N/m^{2})  Density  ρ  (kg/m^{3}) 

Water (10^{o}C)  2.09  999.7 
Oil  1.35  920 
Ethyl Alcohol  1.06  810 
Mercury  28.5  13595 
 properties at 1 bar and 0 ^{o}C
Speed of Sound  Sonic Velocity  in Ideal Gases
Since the acoustic disturbance introduced in a point is very small the heat transfer can be neglected and for gases assumed isentropic. For an isentropic process the ideal gas law can be used and the speed of sound can be expressed as
c = (k p / ρ)^{1/2}
= (k R T)^{1/2} (3)
where
k = ratio of specific heats (adiabatic index)
p = pressure (Pa, psi)
R = individual gas constant (J/kg K, ft lb/slug ^{o}R)
T = absolute temperature (^{o}K, ^{o}R)
For an ideal gas the speed of sound is proportional to the square root of the absolute temperature.
Example  Speed of Sound in Air
The speed of sound in air at 0 ^{o}C (273.15 K) and absolute pressure 1 bar can be calculated as
c = (1.4 (286.9 J/K kg) (273.15 K))^{1/2}
= 331.2 (m/s)
where
k = 1.4
and
R = 286.9 (J/K kg)
The speed of sound in air at 20 ^{o}C (293.15 K) and absolute pressure 1 bar can be calculated as
c = (1.4 (286.9 J/K kg) (293.15 K))^{1/2}
= 343.1 (m/s)
Example  Speed of Sound in Water
The speed of sound in water at 10 ^{o}C can be calculated as
c = ((2.09 10^{9 }N/m^{2}) / (999.7 kg/m^{3}))^{1/2}
= 1446 (m/s)
where
E_{v}= 2.09 10^{9} (N/m^{2})
and
ρ = 999.7 (kg/m^{3})
 Speed of Sound in Water  Speed of sound in water at different temperatures  imperial and SI units.
Speed of Sound in Solids
 Speed of Sound in common Solids
 Elastic Properties and Young Modulus for some Materials
 The Bulk Modulus for Elasticity
 Material Properties
Subsonic and Supersonic speed
 If the Mach Number is below 1, the flow velocity is lower than the speed of sound  and the speed is subsonic.
 If the Mach Number is 1  the speed is transonic.
 If the Mach Number is above 1, the flow velocity is higher than the speed of sound  and the speed is supersonic.
Related Topics

Acoustics
Room acoustics and acoustic properties, decibel A, B and C, Noise Rating (NR) curves, sound transmission, sound pressure, sound intensity and sound attenuation. 
Fluid Mechanics
The study of fluids  liquids and gases. Involving velocity, pressure, density and temperature as functions of space and time.
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