John Doe wrote:
The speed with which sound waves in the air pass a stationary observer
depends on the
{*Where* did you find this stuff?]
(A) speed of the air relative to the observer
"Stationary" in the context of discussions of the speed of sound
usually means 'stationary with respect to some fixed frame of
reference.' This is not necessarily true of the air. Wind can affect
the apparent speed of sound of air relative to the observer.
(B) speed of the source relative to the air
This results in a doppler frequency shift, not in a change of the speed
of sound.
(C) frequency of the source
Frequency is independent of velocity - at least in the range of what is
normally called sound.
(D) wavelength of the sound in the air
Wavelength is also independent of speed. The *product* of frequency
and wavelength equals speed.
(E) intensity of the sound in the air
Unless the intensity of the sound is so great that the dynamic pressure
varies beyond the limits of an ideal gas (due to heat capacity ratios,
among other things) - the pressure variation is independent of the
velocity.
speed of sound = square root of k*p/air density= square root of k*R*T/M
K (kappa) = adiabatic index
T = absolute temperature
R = constant
kappa is the heat capacity ratio - C(p) / C(v) - the ration of the heat
capacity at constant pressure to the heat capacity at constant volume.
This is also called the adiabatic index, and directly affects the way
the gas responds to pressure changes that are too fast to allow thermal
equilibration.
if medium is solid it also depends on stiffness.
"Solid" air - now *that* would be an interesting research material.
I don't see any of these varibles in one of the answer choices.
Look here:
http://scienceworld.wolfram.com/physics/SpeedofSound.html
Tom Davidson
Richmond, VA
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