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#1 | |
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diyAudio Member
Join Date: Jan 2004
Location: Toronto, ON, Canada
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... a diaphragm enters breakup?
http://www.linkwitzlab.com/x-mid_dist.htm Quote:
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#2 |
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diyAudio Member
Join Date: Aug 2004
Location: Behind you
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The quote is correct, but it's a different mechanism to breakup. What the quote describes is that the limited speed of sound in air means that, off-axis, sound radiating from opposite sides of the cone will no longer be in phase as the wavelength approaches the size of the cone. This means that a driver will start to become directional at higher frequencies, instead of radiating spherically.
On the other hand, breakup of a cone occurs near various resonant modes of the cone. The result is a very peaky frequency response at those frequencies. It depends on the geometry and material of the cone, and is not something that a DIYer would be able to calculate.
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#3 |
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diyAudio Member
Join Date: Jun 2004
Location: New Orleans, LA
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Going back to GA Briggs in the 50's, it does seem that in general you can expect a first severe break-up from an 8" paper cone driver at around 3.5 to 4 KHz.
There's no doubt whatsoever that geometry and material properties play a huge role, but driving a cone from the center with a compliant edge mount does tend to limit the range of possibilities. |
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#4 |
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diyAudio Member
Join Date: Nov 2003
Location: Brisbane, QLD
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I think many people could be quite surprised at how low the break-up frequencies can be. In the picture of Vifa's measurement of their TC14WG49-08 speaker which is only 5.5 inches, I'd estimate the first severe break-up mode to be at about 1.1kHz-1.3kHz. The glitch may be next-to invisible considering the flatness of the frequency response, and there are only 2 small clues that suggest cone break-up:
1) A very small change in frequency causes a relatively large ripple in the amplitude response - ie: a high-Q notch or bandpass filter. 2) There is a small peak in the impedance plot caused by a sudden change in the effective mass of the cone. |
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