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person123
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- TL;DR Summary
- While higher frequencies seem to generally dissipate more than lower frequencies (e.g. sound waves, vibrating strings), the opposite is the case for shallow water waves: why might this be the case?
In general, it seems that higher frequencies of a wave dissipate more than lower frequencies.
For sound waves, it explains why you can hear lower pitches from farther away. For a vibrating string or plate, the higher frequencies also dissipate first, with the fundamental fading last. For water sloshing in a container (say a cup), the fundamental, main sloshing, is also what remains. In the case of light, the greater scatter of higher frequencies explain why the sky is blue (maybe this doesn't count because it's not really dissipation though).
There is an exception though -- traveling shallow water waves. It is well established (from experimental, field, and numerical work), that when a wave passes an obstacle like an underwater reef (and so energy is dissipated) the lower frequencies die out but the higher frequencies actually increase in amplitude. It's also sort of intuitive -- it seems reasonable that a sinusoidal water wave would get morphed into messier, higher frequency waves on passing an obstacle.
Why does this break the rule? Is there anything to get out of it being reversed?
For literature on this from the linked paper:
"Generation of higher harmonics in waves propagating over submerged obstacles has long been known. Johnson et al. (1951 ) noted that over natural reefs the energy was transmitted as a multiple crest system. Jolas (1960) carried out experiments with a submerged obstacle of rectangular cross section and observed that the transmitted waves were noticeably shorter than the incident waves. In an experimental study investigating the performance characteristics of submerged breakwaters, Dattatri et al. ( 1978 ) pointed out rather complex forms of the transmitted waves, which indicated the presence of higher harmonics. Drouin and Ouellet ( 1988 ) and Kojima et al. (1990) reported their experimental results with immersed plates, the latter emphasizing the phenomenon of wave decomposition and associated harmonic generation past the obstacle. Quite recently, Rey et al. ( 1992 ) have reported similar results for laboratory waves passing over a bar."
For sound waves, it explains why you can hear lower pitches from farther away. For a vibrating string or plate, the higher frequencies also dissipate first, with the fundamental fading last. For water sloshing in a container (say a cup), the fundamental, main sloshing, is also what remains. In the case of light, the greater scatter of higher frequencies explain why the sky is blue (maybe this doesn't count because it's not really dissipation though).
There is an exception though -- traveling shallow water waves. It is well established (from experimental, field, and numerical work), that when a wave passes an obstacle like an underwater reef (and so energy is dissipated) the lower frequencies die out but the higher frequencies actually increase in amplitude. It's also sort of intuitive -- it seems reasonable that a sinusoidal water wave would get morphed into messier, higher frequency waves on passing an obstacle.
Why does this break the rule? Is there anything to get out of it being reversed?
For literature on this from the linked paper:
"Generation of higher harmonics in waves propagating over submerged obstacles has long been known. Johnson et al. (1951 ) noted that over natural reefs the energy was transmitted as a multiple crest system. Jolas (1960) carried out experiments with a submerged obstacle of rectangular cross section and observed that the transmitted waves were noticeably shorter than the incident waves. In an experimental study investigating the performance characteristics of submerged breakwaters, Dattatri et al. ( 1978 ) pointed out rather complex forms of the transmitted waves, which indicated the presence of higher harmonics. Drouin and Ouellet ( 1988 ) and Kojima et al. (1990) reported their experimental results with immersed plates, the latter emphasizing the phenomenon of wave decomposition and associated harmonic generation past the obstacle. Quite recently, Rey et al. ( 1992 ) have reported similar results for laboratory waves passing over a bar."