Measuring temperature profiles

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SUMMARY

This discussion focuses on the simulation of temperature profiles in a thermoacoustic refrigerator, specifically using Fluent for 2D simulations. The project involves a resonator tube with a loudspeaker and a stack that creates a temperature gradient. Participants concluded that while temperature should theoretically follow pressure profiles in standing waves, it is affected by absolute measurement differences and thermal conductivity, leading to discrepancies in simulation results. The conversation emphasizes the importance of accurate representation of variables in simulations and suggests comparing results with experimental data for validation.

PREREQUISITES
  • Understanding of thermoacoustic refrigeration principles
  • Familiarity with Fluent for fluid dynamics simulations
  • Knowledge of standing wave behavior in resonator tubes
  • Basic concepts of heat transfer and thermal conductivity
NEXT STEPS
  • Research the impact of thermal conductivity on temperature distribution in resonator tubes
  • Learn about the mathematical modeling of standing waves in acoustics
  • Explore advanced simulation techniques in Fluent for accurate temperature profiling
  • Investigate experimental methods for validating simulation results in thermoacoustic systems
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Engineers, physicists, and researchers involved in thermoacoustic refrigeration, fluid dynamics simulation, and heat transfer analysis will benefit from this discussion.

Tsunami
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Here's the thing. This year we had to work on a project, mine's about building a thermoacoustic refrigerator. I'll first give some background, for those who are not familiar with it, and believe they need to know these details to answer my question:

Essentially, it's made of the following component:
a resonator tube, closed at one end, and half a wavelength long;
a loudspeaker, set at the other end, in such a way that it more or less behaves like a closed end of the tube, and sending in an acoustic pressure wave operating at resonant frequency; (so, a standing wave is created)
last element is a stack, an element of small solid layers placed into the tube --the thermal contact between the stack layers and the fluid (which is air) evokes a temperature gradient over the two sides of the stack, and thus a heat pump is made (and of course, if you have a heat pump you can have refrigeration).

A part of this project involves simulating the velocity stream function and temperature profile of the waves in this resonator tube, and comparing them to the streaming and temperature profile of a resonator tube without stack, and closed at both ends. These simulations are done in 2D (there is axial symmetry) in Fluent.

When I look at the velocity stream function of the closed tube without stack, I get vortex streaming (eddies) as expected - there are 2 times 2 eddies, placed symmetrically about the longitudinal axis and also mirrored around the centre of the tube.

When I look at the temperature profile (plotted against the longitudinal distance), I get something that looks more or less like a cosine, with its minimum in the centre of the tube.
Now, I think that's a bit funny. When you have a standing pressure wave in your tube:

p = P1 cos(omega*t-k*x) +P0 , P0 being p_atmosphere

You should get a pressure profile that looks like (for t=0):

p= P1 | cos(k*x) | in absolute value . This is right, yes?

They told me it's like this because the pressure you measure is simply the difference with reference pressure, and it doesn't matter if it's a greater or a lower pressure.

Now, since temperature follows pressure, shouldn't I get a temperature profile that looks like:

T= T1 |cos(k*x)| ?

... I've been thinking a whole number of things:

1. for temperature it's different than pressure, you don't measure in relation to your reference, you simply measure its value;
2. the fact that you can't measure negative pressure is a measurement problem, but the relative pressure amplitude itself does become negative.
3. My simulation is simply wrong.

Maybe it's a good thing to mention that there is a good reason to doubt that my simulations are reliable. :shy:
 
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You know more about what you are talking about than I do, but let me throw out some observations. If they make any sense to you, great; if not you can ignore them :smile:
p = P1 cos(omega*t-k*x) +P0 , P0 being p_atmosphere
This does not look right to me. Assuming P1 is a constant, this would represent a traveling wave. What you should have for a standing wave is a spatial profile multiplid by a time dependent sinusiod. If x = 0 is the driving end, and the location of maximum pressure variation, the spatial profile would be something like cos(kx), with k chosen to give you a node at the closed end of the tube. That would be modulated by the time varying function. So I think you should have something like

p = P1 cos(k*x)*cos(omega*t) +P0 , P0 being p_atmosphere

At t=0, this becomes your next equation, but there is no need for the absolute value for a half-wavelength tube. You would want it for higher order harmonics.

Actually, I think maybe your tube is a quarter wavelength with the speaker driver at the open end being an antinode, as illustrated here,

http://hyperphysics.phy-astr.gsu.edu/hbase/waves/clocol.html#c1

but it would not have to be. The speaker end could be near a node of a half wavelength tube that would have an antinode in the middle. That seems to fit better with your comparison tube that is closed at both ends. If that is the case, the spatial function would have to be in terms of x = 0 in the middle of the tube. Alternatively, the spatial function could be a sine function that has zeros at both ends of the tube.

As for the temperature following the pressure, I think you are on the right track. This article seems to be what you are talking about, though it apperas to me they are working with a quarter wavelength tube. It explains the heat pumping process you are dealing with

http://www.americanscientist.org/template/AssetDetail/assetid/21006/page/2#23065
 
Last edited:


First of all, great job on your project and congratulations on successfully building a thermoacoustic refrigerator! Now let's dive into the issue of measuring temperature profiles.

You are correct in thinking that the temperature profile should follow a similar pattern as the pressure profile, since temperature is directly related to pressure in a standing wave. However, there are a few factors to consider when measuring temperature profiles in this scenario.

Firstly, as you mentioned, temperature is an absolute measurement, whereas pressure is a relative measurement. This means that a negative temperature value does not make sense, unlike a negative pressure value. Therefore, the temperature profile cannot simply mirror the pressure profile.

Secondly, the temperature profile is also affected by other factors such as heat transfer and thermal conductivity of the materials involved. These factors can alter the temperature distribution and may not necessarily follow the same pattern as the pressure profile.

Lastly, as you mentioned, there is a possibility that your simulations may not be entirely accurate. It is important to consider all the variables and factors involved in your experiment and make sure they are accurately represented in your simulation. It may also be helpful to compare your simulation results with experimental data to ensure their reliability.

In conclusion, while the temperature profile may not exactly mirror the pressure profile in a standing wave, it is important to consider the various factors that may affect its distribution. Keep in mind that temperature is an absolute measurement and may not behave in the same way as pressure. Good luck with your project!
 

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