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#341 |
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diyAudio Member
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As for the third strategy I'm curious what will happen if you take such a foam:
http://apama.pl/APAMA%20FOTOS/PANEL%...T7.5.200-1.JPG spray with a stiff resin and excite transversely and longitudinally. |
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#342 |
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diyAudio Member
Join Date: Mar 2008
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Hi,
for me the link does not work, could you post a picture please ? Maybe there was a misunderstanding concerning my former post: I do not think that it is very useful to increase modal density at low frequencies by searching for materials only. I'd like to do it by design ... But i am curious concerning that foam ... |
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#343 |
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diyAudio Member
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The idea is as follows - generate longitudinal waves like in yours plus transverse and if they are shorter than panel dimension then radiation like above fc occurs. Below bending waves are excited on pyramids - "wide coincidence region". Radiation will be efficient but the question is if f0 are not higher than in a plain membrane.
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#344 | |
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diyAudio Member
Join Date: Mar 2008
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Quote:
"Below" means below concidence frequency or below the range where (bending) wavelength is in the range of panel dimension ? What do you mean with "excited on pyramids" ? What kind of motion do you intend for a single pyramid e.g. ? |
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#345 |
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diyAudio Member
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I mean the torsion motion on the edges, radiation below coincidence. You can check it with your transducer just compare curved membrane with a flat one. Curved will be more efficient. Bending waves forms around exciter and edges so more "knees" you have more the longitudinal waves are transformed into bending transverse waves.
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#346 | |
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diyAudio Member
Join Date: Mar 2008
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Quote:
do you mean the "small scale" curvature introduced by pyramids (crumbles, ripples) on a structured surface ? My transducer has both, but the "small scale" curvature (ripples) is small against bending wave length ( at least up to the mid frequency range). |
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#347 |
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diyAudio Member
Join Date: Mar 2008
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What about "fractal folded" strucure ...
Of cause the structure below is not fractal enough By that you introduce - larger surface - length of possible propagation paths increases and is randomly "smeared" over neighboured paths - stiffness, mass and speed of bending waves will vary regionally and is path dependent, thereby varying along each single path. I think this is what i have already to some extent in my transducer, although it is not really "fractal". |
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#348 |
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diyAudio Member
Join Date: Mar 2008
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#349 |
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diyAudio Member
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Any change in curvature, bending stiffness generate bending waves. Please have a look again (page 14+):
http://www.wikipatents.com/gb/2400264.html |
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#350 |
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diyAudio Member
Join Date: Mar 2008
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That is understood, but i thought we were discussing
- how to increase modal density by structure (not overall size) - some idea of "broadband" coincidence ??? Your foam with pyramids was an attempt to go into that direction. I just tried to understand your idea, while finding it interesting ... I am currently thinking about a different approach to increase modal density in the lower frequency range of a DML, which does not necessarily imply curvature of any scale. |
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