Math in not coarse. Think about calculating pi. 3.14159 26535 89793 23846 26433 83279 50288 41971 69399 37510 ...
Math is used to describe energy. motion, and all manner of forces, even dark energy.
By using your logic, sound will propagate faster in colder and more highly pressurized air, (continuing to stick with air). It doesn't. Colder air is denser as is pressurized air. But, sound travels slower in colder air and the pressurization has little or no effect on the speed. There must be some other mechanism at work as regards sound propagation.
Finally, after you think about it, go back to the wave analysis model and tell me how "longitudinal waves", generated by some subsonic disturber (such as vocal cords, a speaker or a steamship whistle) virtually instantly accelerate to Mach 1 and propagate at that speed.
This is indeed true, i'm sorry for putting it this way. let me put it in a way that makes some semblance of sense. When I said density, it is a combination of the velocity of the particles in the medium (directly affected by by temperature) and for want of of a better word the compressibility of the medium.
By compressibility I mean the relative distance that the particles can get to one another. This variable would be directly related to the intermolecular forces present in the medium
With lower compressibility (particles cannot get as close to each other) the sound would propagate faster.
I think somewhere I saw the analogy used that a lower compressibilty is akin to having stiffer springs. Whilst the energy transferred is the same, the rate of transferral is much quicker when the compressibility is lower (stiffer spring).
This would indicate, assuming sound is dependent on the kinetic interactions between the molecules, that sound would indeed travel slower in a cooler air than hotter air.
Your mode of operation is to write off anything that is above your level of comprehension. I will go with Feynman!crashsite said:When I see or hear someone touting the demigod, Feynman and professing that mathematics is the "language of the universe", I just wince.
Why would you include the temperature (velocity) of the molecules as part of the definition of, "density"? I looked up, "density" and there's nothing in any of the definitions that even suggests a dynamic aspect:
But, now let's take the same tank of air but, instead of raising the temperature, you add more air to increase the pressure. The air molecules are pushed closer together and, even though their thermal activity is lower, there will be a greater interaction (more stiffness) between the molecules because they are simply in closer proximity.
In the second case I came up with, there is a "same stiffness" between the molecules but, it takes more molecules to acheive it. For a disturbance to pass through the molecules is still dependent on the intermolecular stiffness and that determines the rate of propagation from molecule to molecule. But, since the disturbance must interact with more molecules to get from point A to point B, it takes longer. Ergo, slower rate of propagation.
So the highest frequency sound in air is 3.4GHzThe highest (effective) frequency that can exist is linked to the
mean free path. This at sea level is about 10^-7m. Hence the highest
frequency (even loosly defined as sound) is 340e7 Hz. Even that is
stretching a point.
I take from this that in the real world >1MHz isn't of much use.The speed and attenuation of sound 2.4.1
gives a general account of attenuation. At 100kHz we have about
1800dB/km in fairly dry air. Attenuation on a simple model goes up as
f^2. Range of 1000kHz therefore bein of the order of 10m (1.8dB/m). At
1MHz we have 10cm. At 10MHz 100 microns. In my book 100MHz+ can't
really exist in air.
gives a general account of attenuation. At 100kHz we have about
1800dB/km in fairly dry air. Attenuation on a simple model goes up as
f^2. Range of 1000kHz therefore bein of the order of 10m (1.8dB/m). At
1MHz we have 10cm. At 10MHz 100 microns. In my book 100MHz+ can't
really exist in air.
I take from this that in the real world >1MHz isn't of much use.
The key to this is the relative distance between the particles. If you increase the pressure by large amounts, i.e doubling, I would presume that there would be a difference. All my reasoning comes not from experimental data but from the perspective of a 17 year old. I have seen somewhere that the speed of sound is only minimally affected by the pressure, but I don't know to what extent. Even the minimal effect that is seen would indicate that there is some sort of interaction which affects the speed of sound due to the proximity of the molecules.
Explains why sound is faster in desnser air. Denser air allows the molecules to collide faster thus increasing the speed of sound.
The reason is easily understood by doing a control volume analysis, i.e. analyzing F = ma on the air in a fixed but otherwise arbitrary region of space. The resistance to compression, which is called the bulk modulus is given by κp where κ is the adiabatic coefficient (ratio of specific heats) and p is the ambient pressure. The density of the gas, ρ, is given by Mp/RT were M is the molecular weight of the gas, R is the universal gas constant and T is the absolute ambient temperature. The square of the speed of sound is given by the ratio of bulk modulus to density and the p's cancel. So as the pressure increases the air acts like a stiffer spring creating more restoring force, but the mass to be accelerated also increases in exactly the same way resulting in no pressure effect.
Skyhawk provided that information and you ignored it.crashsite said:That's just it. Even with large pressure changes, the speed of sound is virtually unchanged.
Either you are not reading or not understanding.skyhawk said:So as the pressure increases the air acts like a stiffer spring creating more restoring force, but the mass to be accelerated also increases in exactly the same way resulting in no pressure effect.
Once again you have overlooked useful information.
A few posts ago you asked why pressure/altitude did not make much of a difference.
Skyhawk provided that information and you ignored it.
Either you are not reading or not understanding.
3v0
I can take some voltage, current and resistance and assign them to the variables E, I and R, respectively. Then I can show that, if I use the formula E=IR that the voltage is proportional to the product of current times resistance. Unfortunately, what I haven't done is explain anything about E, I or R or what they are or consist of or how to concptualize them except as they numerically relate to each other. For someone who wants to know how electricity works but, isn't particularly interested in actually designing a circuit, the info I've given is useless.
Math needs to be the slave that supports the concept. Not the master that dictates how it must be viewed.
Yes, I can hear the heavy sighs...
Once again you have overlooked useful information.
A few posts ago you asked why pressure/altitude did not make much of a difference.
Quote:
Originally Posted by crashsite
That's just it. Even with large pressure changes, the speed of sound is virtually unchanged.
Skyhawk provided that information and you ignored it.
Either you are not reading or not understanding.
What you've stated is a huge simplification of Ohm's law, I'm not surprised that it's not enlightening. If you want to understand the concepts described by Ohm's law then use Maxwell's equations and derive Ohm's law and I guarantee you that you'll understand exactly how Ohm's law works and what it is conceptually.
My point is that most of the mathematics that are used to describe nature started out as experiments similar to this thread. Once the mechanics were thoroughly understood they were simply translated to mathematics. There are dozens of examples of these, quite rarely did mathematicians have anything to do with it. Most times it was practitioners that were interested in finding out more. Faraday and Ampere are two such examples. Using mathematics is a convenient way to express the results of the experment.
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