Speed of sound - why does adding ethanol to water increase the speed of sound

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Discussion Overview

The discussion focuses on the phenomenon of the speed of sound in ethanol-water mixtures, exploring why the addition of ethanol to water appears to increase the speed of sound. Participants examine theoretical calculations, empirical data, and potential discrepancies in measurements, with a focus on the physical properties of the liquids involved.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that the speed of sound in pure water is approximately 1482 m/s and question why adding ethanol, which has a lower speed of sound in isolation, would increase the overall speed in a mixture.
  • One participant provides calculations for the speed of sound in both water and ethanol, suggesting that the speed in ethanol is slower than in water, raising doubts about the initial claim.
  • Another participant references a paper that includes empirical data on the speed of sound in ethanol-water mixtures, providing specific values for different concentrations of ethanol.
  • Some participants express reluctance to access the referenced paper due to cost, while others share links to alternative resources that discuss the bulk modulus and density of mixtures.
  • A participant presents a mathematical derivation for the speed of sound in mixtures, indicating that the speed should decrease with increasing ethanol concentration based on their calculations.
  • Discrepancies in the reported speed of sound values from the referenced paper are discussed, with participants attempting to reconcile these with their own calculations.
  • Concerns are raised about the temperature dependence of the speed of sound in water and mixtures, with one participant suggesting that temperature variations could affect the results significantly.
  • There is a discussion about the grade of ethanol used in the experiments, with questions about whether it was absolute or anhydrous ethanol, which could influence the physical properties and resulting speed of sound.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the reasons for the observed increase in speed of sound with ethanol addition. Multiple competing views and calculations are presented, leading to an unresolved discussion regarding the underlying physics and empirical data.

Contextual Notes

Participants highlight the importance of temperature on the speed of sound in water and mixtures, noting that the density and bulk modulus of the liquids can vary significantly with temperature. There are also discussions about the definitions of volume percentages in mixtures, which may affect calculations.

Who May Find This Useful

This discussion may be of interest to those studying fluid mechanics, acoustics, or physical chemistry, particularly in relation to the properties of liquid mixtures and sound propagation.

lavster
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If you have a tank of water then the speed of sound is 1482 m/s. If you add ethanol, the speed of sound increases. This seems to be pretty linear with the % concentration of ethanol. why does ethanol (or propanol) increase the speed of sound?

thanks
 
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lavster said:
If you have a tank of water then the speed of sound is 1482 m/s. If you add ethanol, the speed of sound increases. This seems to be pretty linear with the % concentration of ethanol. why does ethanol (or propanol) increase the speed of sound?

thanks

Can you please post the reference document for the above? This may help members in their effort to answer your query. Thank you.

Cheers,
Bobbywhy
 
This seems rather strange.

Water: density 1000 Kg/m^3, bulk modulus 2.2 GPa
Speed of sound = sqrt(2.2/1.0) * 1000 = 1480 m/s, as you said.

Pure ethanol: density 789 Kg/m^3, bulk modulus 1.07 GPa
Soeed of sound = sqrt(1.07/0.789) * 1000 = 1164 m/s
which is slower than in water, not faster :confused:
 
I can see the graph, but I'm not going to pay money to read the paper - sorry!
 
AlephZero said:
I can see the graph, but I'm not going to pay money to read the paper - sorry!

I also.
 
I found the following link (see the section Bulk modulus of mixtures 1.6.2.1)
http://www.scribd.com/doc/51230908/46901640-Fluid-Mechanics#page=80

If you look at Eqn.(1.42), you will find that:
<br /> B_{\mathrm{mix}} = \frac{1}{\frac{x_1}{B_{1}} + \ldots + \frac{x_n}{B_n}}<br />
where x_i = V_i/V are the volume fractions of each component.

A similar derivation will convince you that the density of a mixture is:
<br /> \rho_{\mathrm{mix}} = x_1 \, \rho_1 + \ldots + x_n \, \rho_n<br />

Now, suppose we have two liquids with volume fractions x, and 1 - x. Then the speed of sound in the mixture is:
<br /> \begin{array}{l}<br /> c_{\mathrm{mix}} = \sqrt{\frac{B_\mathrm{mix}}{\rho_\mathrm{mix}}} = \sqrt{\frac{\frac{1}{\frac{x}{B_1} + \frac{1 - x}{B_2}}}{x \, \rho_1 + (1 - x) \, \rho_2}} \\<br /> <br /> = \sqrt{\frac{B_1 \, B_2}{\left[ x \, B_2 + (1 -x) \, B_1 \right] \, \left[ x \, \rho_1 + (1 - x) \, \rho_2\right]}} \\<br /> <br /> = \sqrt{\frac{B_2}{\rho_2} \, \frac{1}{ \left[ 1 + \left( \frac{B_2}{B_1} - 1 \right) \, x \right] \, \left[ 1 + \left( \frac{\rho_1}{\rho_2} - 1\right) \, x\right]}}<br /> \end{array}

At very low fractions x, we may expand this expression in powers of x, and the first two terms in the expansion are:
<br /> c_\mathrm{mix} = c_2 \, \left[ 1 + \left(-\frac{1}{2}\right) \, \left(\frac{B_2}{B_1} - 1 \right) \, x + o(x)\right] \, \left[ 1 + \left(-\frac{1}{2}\right) \, \left(\frac{\rho_1}{\rho_2} - 1 \right) \, x + o(x)\right]<br />
<br /> c_\mathrm{mix} = c_2 \, \left\lbrace 1 + \left[1 - \frac{1}{2} \, \left(\frac{B_2}{B_1} + \frac{\rho_1}{\rho_2} \right) \right] \, x\right\rbrace<br />
Now, in post #3, we were given the info:
<br /> \frac{B_2}{B_1} = \frac{2.2}{1.07} = 2.06<br />
<br /> \frac{\rho_1}{\rho_2} = \frac{789}{1000} = 0.789<br />
So, the coefficient in front of x is:
<br /> 1 - \frac{2.06 + 0.789}{2} = 1 - 1.423 = -0.423<br />

It corroborates the poster's conclusion that the mixture's speed of sound should decrease with volume fraction of ethanol.

If you have access to the paper, could you post the relevant plot where increase is shown?
 
To see the plot, click the link in post #4. The values at the ends of the plotted range are
1519 m/s for 6% ethanol
1558 m/s for 12%

I might have used the wrong bulk modulus of ethanol.

http://www.efunda.com/materials/common_matl/show_liquid.cfm?MatlName=AlcoholEthanol gives 0.823GPa for ethanol at 20C and 2.18 for water at 20C.

But the numbers still don't agree. For 6% ethanol
Modulus: 1/B = 0.94 / 2.18 + 0.06 / 0.823
B = 1.983 GPa
density = 0.94 x 1000 + 0.06 x 789 = 987 kg/m^3
Speed of sound = sqrt (1.983/0.987) x 1000 = 1417 m/s
which is less than water, and not consistent 1519 on the graph.
 
I have access to the paper. I don't know if I am allowed to upload the pdf.

Just to make sense of some of the number discrepancies we are getting, let me refer to their Table 1 for the temperature dependence of water in distilled water:

attachment.php?attachmentid=51121&stc=1&d=1348362279.png

The cited source for the first column is:
V. A. Del Grosso and C. W. Mader, J. Acoust. Soc. Am. 52, 1442-1446 (1972)
(I think the access to this paper is free)

The second column, of course, are the measurements by the authors of the paper we are considering.

Apparently the speed of sound in water is highly dependent on temperature.

From Fig.3 of the graph (the one linked in post #4), AlephZero deduced:
AlephZero said:
To see the plot, click the link in post #4. The values at the ends of the plotted range are
1519 m/s for 6% ethanol
1558 m/s for 12%
which would imply a speed of sound for pure water:

1519 + (0 - 6)*(1558-1519)/(12 - 6) = 1519 + (-6)*39/6 = 1480 m/s

Looking at the Table 1, this would correspond to a temperature:

19.9 + (1480-1481.4)*(19.9-18.0)/(1481.4-1475.1) = 19.9 + (-1.4)*1.9/5.7 = 19.9 - 0.47 = 19.4 oC

which is different from the quoted 20o C by 0.6 Co, a three times larger difference than the quoted temperature accuracy

The temperature of the medium was controlled by a laboratory heater/stirrer and measured with a calibrated platinum resistance thermometer (ETI Ltd, Worthing, UK) with an accuracy of ±0.2°C.

Maybe they had some issues with temperature stability of the mixtures.
 

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  • #10
Dickfore said:
Apparently the speed of sound in water is highly dependent on temperature.

Sure, if only because the density variies significantly with temperature.

But it would be surprusing if the variation in speed of the mixsture went different ways at different temperatures. Fractions of a degree C shouldn't make much practical difference.

Do they give any properties for ethanol? With the numbers I used, the reduced speed matches "common sense". Addiong a small amount of ethanol reduces the bulk modulus a lot (reducing the speed a lot) and reduces the dessity a little (increasing the speed a little), so the net effect is a reduction.

I'm wondering what grade of ethanol those properties are for - absolute (abut 4% water content), anhydrous, or something else.
 
  • #11
AlephZero said:
I'm wondering what grade of ethanol those properties are for - absolute (abut 4% water content), anhydrous, or something else.

This is a quote from their paper:
Measurements of c were made over a range of temperatures in mixtures of ethanol (99.7% v/v min, Hayman Ltd, Witham, Essex, UK) in freshly distilled water. Ethanol concentrations of 6%, 8%, 10% and 12% by volume were used. The estimated uncertainty in the concentration was ±0.1%.

EDIT:
This may shed some light on the mystery:
Volume %

The Volume % is bit strange in that the Volume % of ethanol and the Volume % of water add up to more than 100. The way the Volume % of ethanol is defined is that it is the parts of ethanol to which water has been added to bring the volume to a total of 100 parts.

For example, when working at 20°C, if you took 48.00 liters of pure ethanol you would find that you would have to add 55.61 liters of water to bring the total volume to 100.00 liters. The Volume % of ethanol in this case is 48.00% and the Volume % of water is 55.61%. The total of the separate components is 103.61 liters, but has contracted to 100.00 liters.

The degree of contraction is affected by the relative quantities ot ethanol and water, and also by the temperature. For example, when working at 50°F you would find that if you again started with 48.00 liters of ethanol you would need 55.82 liters of water to bring the total to 100.00 liters. This means that when a strength is specified in Volume % the temperature has to be specified as well.

Ethanol has a significantly higher coefficient of expansion than water. This means that as the temperature varies, the volume of the ethanol portion of the mixture changes faster than that of the water portion.

Does anyone know what kind of a unit "v/v min" is?
 
Last edited:
  • #12
Dickfore said:
Does anyone know what kind of a unit "v/v min" is?

I would take v/v as "volume / volume", i.e. the spec means "minimum 97.7% ethanol by volume", as opposed to "by mass".

The volume contraction effect they mention probably affects the bulk modulus of the mixture as well, which makes the short answer to the OP's question "The reason isn't simple".

The relationship can't be linear over the full range from 0% to 100% ethanol, unless somebody can make an argument that ##c = \sqrt{K/\rho}## doesn't apply to pure ethanol.
 
  • #13
wow - thanks everyone! glad I am not missing something really obvious! your help is much appreciated!
 

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