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Calculation formulas for the speed of sound in gases, fluids and solids.
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An consequence of the compressibility of gases, fluids and solids, is that disturbances introduced in some point will propagate at a finite velocity.
The velocity at which these small disturbances will propagate through the medium is called the Acoustic Velocity or the Speed of Sound.
Acoustic velocity can be expressed as:

In equation (1) the speed of sound is related to changes in pressure and density of the fluid.
In equation (2) the speed of sound is in terms of the Bulk Modulus for Elasticity and density of the medium. This equation is valid for liquids, solids and gases. The sound will travel faster through media with higher elasticity and lower density. If the medium is not compressible at all - incompressible - the speed of sound is infinite (c ≈ ∞).
| Medium Properties at 1 bar and 0 oC | Bulk Modulus for Elasticity Ev (N/m2) | Density ρ (kg/m3) |
| Water | 2,06 109 | 999,8 |
| Oil | 1,35 109 | 920 |
| Ethyl Alcohol | 0,94 109 | 810 |
| Mercury | 28,5 109 | 13.595 |
Since the disturbances introduced in some 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 (3) and (4).
For an ideal gas the speed of sound is proportional to the square root of absolute temperature.
If we have air at 0 oC and the absolute pressure is 1 bar - the speed of sound can be calculated:
c = (1,4 287 273)1/2 = 331,2 (m/s)
where
k=1,4 and R=287 (J/K kg)
If we have air at 20 oC and the absolute pressure is 1 bar - the speed of sound can be calculated:
c = (1,4 287 293)1/2 = 343,1 (m/s)
If we have water at 0 oC - the speed of sound can be calculated:
c = (2,06 109/999,8)1/2 = 1435,4 (m/s)
where
Ev= 2,06 109 (N/m2) and ρ = 999,8 (kg/m3)
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