sophiecentaur
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I also know that the CM of a small mass of gas will accelerate in the direction of the pressure gradient. The pressure gradient in the plane of the wave is zero and also the acceleration (that's referred to as a wave front). Which is why I jumped a step. The pressure and displacement are in time quadrature - just like any other longitudinal wave. Molecular motion is a red herring here - just as with electron motion in a metal; just consider bulk movement of an elemental volume.Dale said:It depends on the initial velocity. You can have motion in any direction with force in any direction, depending on the initial velocity.
In sound you can and do have molecules that are moving in the opposite direction of the pressure gradient. They are accelerating in the direction of the pressure gradient but not moving that direction.
I know that you know the difference between acceleration and velocity.
I don't see why you don't just try the line of masses and springs model as a starter for any longitudinal wave. Google "is sound a longitudinal wave?". How is a longitudinal wave described? You say pressure is in all directions so something must be longitudinal; how about displacement?