Instant accelelation in travelling wave

  • Thread starter Thread starter petermer
  • Start date Start date
  • Tags Tags
    Wave
AI Thread Summary
When a traveling wave approaches a point in a medium, that point remains stationary until the wave reaches it, at which moment the atoms accelerate rapidly to match the wave's speed. This acceleration appears nearly instantaneous from a macroscopic perspective, but it results from intense microscopic collisional activity as the wavefront nears. The atoms do not feel the wave until it is very close, as the wave travels faster than the ambient pressure propagation speed. This phenomenon is an idealization, particularly relevant in shock waves, where the force generated comes from the rapid interactions between atoms. Understanding this process clarifies how forces are transmitted through a medium during wave propagation.
petermer
Messages
15
Reaction score
0
It just occurred to me: when a traveling wave approaches a certain point in the medium, the point remains still. When the wave reaches the point however, it instantly accelerates to maximum velocity. How does this happen? Where does this huge force come from? Is the time needed for the point to get this velocity negligible?
 
Physics news on Phys.org
Are you referring to a discontinuous wavefront traveling through some medium? If so, that's probably just an approximation.

It could be a good appxorimation if you are only considering the system in question on such a large scale that the spread of the wave front can be regarded as zero.

Torquil
 
Yes, as torquil said, that's just an idealization... as the shock wave approaches the stationary atoms, there is a tremendous amount of microscopic collisional activity which very rapidly accelerates those atoms to the speed of the wave. The atoms in front of the wave don't feel the wave until it is already very close, because the wave is traveling faster than the ambient speed of pressure propagation. So there is no instantaneous acceleration, but the atoms are accelerated very rapidly at the last possible moment, and so it looks practically instantaneous from a macroscopic observer.

For an ordinary wave (equal to the sound speed), this dramatic acceleration doesn't occur, of course.
 
Ok, but how is this tremendous force generated from the atoms?
 
Hello! Let's say I have a cavity resonant at 10 GHz with a Q factor of 1000. Given the Lorentzian shape of the cavity, I can also drive the cavity at, say 100 MHz. Of course the response will be very very weak, but non-zero given that the Loretzian shape never really reaches zero. I am trying to understand how are the magnetic and electric field distributions of the field at 100 MHz relative to the ones at 10 GHz? In particular, if inside the cavity I have some structure, such as 2 plates...

Similar threads

Replies
27
Views
2K
Replies
3
Views
2K
Replies
13
Views
3K
Replies
2
Views
1K
Replies
4
Views
2K
Replies
42
Views
4K
Back
Top