Do soundwaves heat up the air through which they travel?

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In thermodynamics, compressional waves in air are typically considered adiabatic, meaning no heat is exchanged with the environment. When sound waves from loudspeakers are isolated, the energy they produce can lead to an increase in air temperature due to the dissipation of sound energy. However, real-world factors such as heat loss to the surrounding walls and energy from electrical components can complicate this scenario. The net effect of sound energy on air temperature depends on the balance between energy dissipation and heat loss. Ultimately, if sound energy cannot escape, it will contribute to heating the air around the speakers.
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I'm doing a problem in thermodynamics that deals with sound waves and the bulk modulus B and it got me thinking. Since the compressional waves would be traveling far too fast to be considered isothermal, I assume you must consider them to be adiabatic compressions of air. Now if adiabatic compression allows no heat to leave the compressed gas, does this mean the temperature of the air would rise? In other words, if I were to totally isolate a set of really loud speakers and leave them blasting for a few hours, would the air around them be noticably hotter? Just looking for some insight on the nature of compressional heating, forgive me if this idea is totally ridiculous (but please tell me why :)).
 
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Conor_McF said:
In other words, if I were to totally isolate a set of really loud speakers and leave them blasting for a few hours, would the air around them be noticably hotter? Just looking for some insight on the nature of compressional heating, forgive me if this idea is totally ridiculous (but please tell me why :)).

Yes, but I bolded 'totally isolate' because in any real experiment you will have heat loss to the walls of the 'room' and also the heat generated by the electrical wiring and the mechanical friction of the speaker head, and these effects will all be much larger by the time the system comes to thermal equilibrium than the contribution of thermal energy to the air from the sound waves.
 
The pressure oscillates so, on average, there is no effect. The only net effect is actually due to the fact that there process isn't exactly isentropic, some energy is dissipated. Of course, all that sound energy must go somewhere. If it cannot escape, it must all be dissipated. So, if you have a loudspeaker producing 100 Watt of power in the form of sound energy and none of that energy leaves the gas, then you must reach some stady state situation in which you end up heating the gas with 100 watt.
 
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Yes, because sound waves attenuate in air; i.e., the sound power level drops off faster than 1/r^2. Here are some attenuation numbers at sea level & STP:

20,000 Hz 528 dB per kilometer
2,000 Hz 9.88 dB per kilometer
200 Hz 0.95 dB per kilometer
20 Hz 0.0127 dB per kilometer

Because the air pressure remains the same before and after, the energy heats the air up.

See http://www.csgnetwork.com/atmossndabsorbcalc.html
 
Count Iblis said:
The only net effect is actually due to the fact that there process isn't exactly isentropic, some energy is dissipated. QUOTE]

Ah, does this have something to do with the process no longer being quasistatic when the compressional speed is comparable to the speed of sound?
 
I vaguely recall an elegant (and obscure) derivation of the speed of sound given the specific heat (maybe vice-versa). I can't seem to find the derivation right now, but it seems to be attached to the names Carnot, Laplace, Huginot, and Hadamard.

IIRC, the assumption is that the process is adiabatic.
 
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