Technical Guides - Speed of Sound in Pure Water
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Bilaniuk and Wong
a) 112 point equation
| c = | 1.40238742 x 103 + 5.03821344 T - 5.80539349 x 10-2 T2 + 3.32000870 x 10-4 T3 - 1.44537900 x 10-6 T4 + 2.99402365 x 10-9 T5 |
b) 36 point equation
| c = | 1.40238677 x 103 + 5.03798765 T - 5.80980033 x 10-2 T2 + 3.34296650 x 10-4 T3 - 1.47936902 x 10-6 T4 + 3.14893508 x 10-9 T5 |
c) 148 point equation
| c = | 1.40238744 x 103 + 5.03836171 T - 5.81172916 x 10-2 T2 + 3.34638117 x 10-4 T3 - 1.48259672 x 10-6 T4 + 3.16585020 x 10-9 T5 |
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T = temperature in degrees Celsius |
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Range of validity: 0-100 °C at atmospheric pressure
Bilaniuk and Wong (1993,1996) converted Del Grosso and Mader's 1972 data to the 1990 International Temperature Scale and then produced three sets of coefficients depending on the number of temperature points which were converted and taken into account in their data fitting routines.
Marczak
| c = |
1.402385 x 103 + 5.038813 T - 5.799136 x 10-2
T2 + 3.287156 x 10-4 T3 - 1.398845 x 10-6 T4 + 2.787860 x 10-9 T5 |
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T = temperature in degrees Celsius |
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Range of validity: 0-95°C at atmospheric pressure.
Marczak (1997) combined three sets of experimental measurements, Del Grosso and Mader (1972), Kroebel and Mahrt (1976) and Fujii and Masui (1993) and produced a fifth order polynomial based on the 1990 International Temperature Scale.
Lubbers and Graaff's simplified equations
a)
A simple equation for use in the temperature interval 15-35°C
| c = | 1404.3 + 4.7T - 0.04 T2 |
Range of validity: 15-35°C at atmospheric pressure. Claimed accuracy - maximum error 0.18 ms-1
b)
| c = | 1405.03 + 4.624 T - 3.83 x 10 -2 T2 |
Range of validity: 10-40°C at atmospheric pressure
Lubbers and Graaff (1998) produced these simple equations with a restricted temperature range for medical ultrasound applications, including tissue mimicking materials and test objects. Within the quoted temperature ranges they claim that the maximum error is approximately 0.18 ms-1 in comparisons with experimental data and more detailed equations such as Bilaniuk and Wong (1993,1996).
Belogol'skii, Sekoyan et al: speed of sound as a function of temperature and pressure
| c(T,P) = | c(T,0) + M1(T)(P - 0.101325) + M2(T) (P- 0.101325)2 + M3(T)(P - 0.101325)3 |
| c(T,0) = | a00 + a10T + a20T2 + a30T3 + a40T4 + a50T5 |
| M1(T) = | a01 + a11T + a21T2 + a31T3 |
| M2(T) = | a02 + a12T + a22T2 + a32T3 |
| M3(T) = | a03 + a13T + a23T2 + a33T3 |
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T = temperature in degrees Celsius P = pressure in megapascals |
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Range of validity: 0-40°C, 0.1 - 60 MPa
This version uses the 1990 International Temperature Scale
Belogol'skii, Sekoyan et al (1999) made their own measurements of sound speed as a function of pressure and temperature and also used the equation of Bilaniuk and Wong (1996) for sound speed at atmospheric pressure.
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Any comments or suggestions about further speed of sound equations?
Please contact Justin Ablitt .