Let's all calm down a little
Nigel, and the others who aren't impressed with the thread:
While i'd make no claims as to the overall quality of the thread (my posts included), i think there is a very important exercise in it. Crashsite (and I, eventually, and maybe others) wanted to understand the propagation of sound on a particle-system level. Since all descriptions of sound we were taught or are able to find on the Internet involve abstracted models of air (the "masses on spring" model), we were at a loss and had to roll our own explanation. This, anyway, became the goal of thread, due to crashsite's apparent allergy to such explanations.
Unlike light, which occupies some nebulous wave/particle duality, air really is particles, and they have well-understood behavior, so it seemed a surmountable challenge. It may be a lot more functional to think of air as masses and springs, or pressure and waves, etc, but we sought a particle-level model that explained why the disturbance propagates at Mach 1, why it's independent of the initial disturbance speed, how the notion of "temperature" as kinetic energy played into it, etc. Even though we are obviously simplifying things a lot, we wanted to at least get together a rough and hopefully intuitive picture of the process.
Despite the low signal/noise, there's value in that.
That's what happens, no doubt. The question was "why". If it's obvious to you on a particle level why and how that happens, and why the system exhibits the counter-intuitive quirks that it does, kudos, and pardon us while we try to figure it out.
Well, it's not an exercise in practicality. It's an attempt to understand a process, not to use it build things.
Respectfully,
-c
Nigel, and the others who aren't impressed with the thread:
While i'd make no claims as to the overall quality of the thread (my posts included), i think there is a very important exercise in it. Crashsite (and I, eventually, and maybe others) wanted to understand the propagation of sound on a particle-system level. Since all descriptions of sound we were taught or are able to find on the Internet involve abstracted models of air (the "masses on spring" model), we were at a loss and had to roll our own explanation. This, anyway, became the goal of thread, due to crashsite's apparent allergy to such explanations.
Unlike light, which occupies some nebulous wave/particle duality, air really is particles, and they have well-understood behavior, so it seemed a surmountable challenge. It may be a lot more functional to think of air as masses and springs, or pressure and waves, etc, but we sought a particle-level model that explained why the disturbance propagates at Mach 1, why it's independent of the initial disturbance speed, how the notion of "temperature" as kinetic energy played into it, etc. Even though we are obviously simplifying things a lot, we wanted to at least get together a rough and hopefully intuitive picture of the process.
Despite the low signal/noise, there's value in that.
Sceadwian said:A transducer displaces a medium, medium compresses, pressure waves move out at the speed of pressure waves in that medium. That's it.
That's what happens, no doubt. The question was "why". If it's obvious to you on a particle level why and how that happens, and why the system exhibits the counter-intuitive quirks that it does, kudos, and pardon us while we try to figure it out.
Sceadwian said:For most practical purposes the actual 'flow' of the molecules of air can be disregarded as inconsequential. [emphasis mine]
Well, it's not an exercise in practicality. It's an attempt to understand a process, not to use it build things.
Respectfully,
-c
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