Sending a sound wave of 1cm wavelength through a 0.1Pascal medium

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Homework Statement
At what pressure (at room temperature) would the mean free path of air molecules reach a macroscopic scale like ##10## cm ? Explain (qualitatively) what would happen if we tried to propagate a sound wave of wavelength ##1## cm in these conditions.
Relevant Equations
$$ l \approx \frac{1}{4 \pi r^{2}}\frac{kT}{p}, $$
I answered the first part of the question where I estimate the radius of ##O_{2}## is ##\approx 1.5 \times 10^{-10} \ \text{m}##:
$$ p = \frac{KT}{l 4 \pi r^{2}} = \frac{(20+273.15)(1.38\times 10^{-23})}{(0.1)(4\pi)(1.5 \times 10^{-10})^{2}} = 0.143 \ \text{Pa}.$$

The confusion arises on the second part of the question. Intuitively I'm thinking that a wave sent through a medium compresses and decompresses periodically the molecules it goes through. If the wavelength is ##1##cm and the mean free path is ##10##cm , then I believe the mean free path will increase by a factor of ##10##? I'm not sure what to think of this problem. Any insights would be appreciated.
 
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Consider a standing wave. Between two nodes, the molecules are bouncing back and forth. What are they bouncing off?
 
haruspex said:
Consider a standing wave. Between two nodes, the molecules are bouncing back and forth. What are they bouncing off?
Sorry , I am not sure to understand the setup. Are they just bouncing off the nodes?
 
Mihail Anghelici said:
Sorry , I am not sure to understand the setup. Are they just bouncing off the nodes?
In a standing sound wave, what is happening at a node in terms of pressure variation and displacement?
 

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