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On 01/12/2015 11:10 AM, Savinainen Antti wrote:
The trouble is, she noted, that sound propagates faster inwater than
in air. This means that there should be no phase change inreflection.
Hence, the incoming and reflected wave should not be out ofphase by
half lambda to create a destructive interference (node).
The wave equation in each medium is characterized by
*two* numbers: the speed of propagation and the impedance.
The reflection from the boundary is characterized by
*two* numbers: the phase and amplitude.
Reflection is controlled by the impedances, not by the
speeds. This is super-easy to demonstrate with electrical
transmission lines. You can have a piece of 50-ohm coax, a
piece of 75-ohm coax, and 300-ohm twinlead all with the same
speed of propagation. There will be humongous reflections
from the interfaces.
There should be a way to visualize this with
mechanical waves but I can't at the moment thing
of a clean and easy way to do it. The air/water
interface exhibits the effect but evidently doesn't
suffice to explain it. Hmmmmm.
Because of the extreme difference in impedance, the
transmission across the air/water interface has a very small
amplitude. You can say whatever you like about the phase,
but it doesn't matter because the amplitude is so small.
By conservation of energy or whatever, if the transmission is
small the reflection must be large.
===================
As a separate matter: Be careful about saying "there is a
node" wherever. At an immovable boundary there will be a
node in the velocity but an /antinode/ in the pressure.
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