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#11 | |
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frugal-phile(tm)
diyAudio Moderator
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Quote:
dave
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community sites t-linespeakers.org, frugal-horn.com, frugal-phile.com ........ commercial site planet10-HiFi p10-hifi forum here at diyA |
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#12 | ||
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diyAudio Member
Join Date: Apr 2007
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Hi,
Quote:
Quote:
Best Baseballbat |
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#13 |
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frugal-phile(tm)
diyAudio Moderator
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But it isn't. Input force decreases by the square of frequency
dave
__________________
community sites t-linespeakers.org, frugal-horn.com, frugal-phile.com ........ commercial site planet10-HiFi p10-hifi forum here at diyA |
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#14 |
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diyAudio Member
Join Date: Dec 2009
Location: Md
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What I have not seen discussed much here is the advantages of forcing materials away from a slab. I have an idea for a low diffraction box of only simple curves. Think about a wide oval cylinder on end with the top a simple curve leading away from the baffle. ( my use case requires it to sit on a shelf, so a round bottom is not viable.) The two edges basically perpendicular to the wavefront. Yes, MDF looks like it will be the material, but laminating several layers of thin hardboard may be better. This is a couple of projects away. Can't say 3/4" MDF is a great material, but I have not had better luck in the 10 to 20L size with other materials. I have no idea where to get that super-duper CF reinforced 9-ply 1/2 inch spruce grown from only north side trees in Norway. I have to deal with what Home Despot sells. I can BUY quarter sheets of MDF which automatically makes it a suitable material.
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#15 |
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diyAudio Member
Join Date: Apr 2007
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hi dave,
you are arguing against Newton's third law. The acceleration of the driver's cone/membran/anything is constant above its resonance frequency*. Otherwise, you wouldn't have a linear frequency response. Thus, the opposing force on the cabinet is constant. There is no mysterious 1/f², only for the energy, but energy is not equal to amplitude (a 1h signal of level 1 has the same energy as a 1 Minute signal of level 60). * In real applications there will be usually a 6 dB down step in acceleration due to the baffle step, so this might be beneficial. Baseballbat |
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#16 |
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frugal-phile(tm)
diyAudio Moderator
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Ues i should have said energy. It is energy that excites the resonance.
dave
__________________
community sites t-linespeakers.org, frugal-horn.com, frugal-phile.com ........ commercial site planet10-HiFi p10-hifi forum here at diyA |
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#17 | |
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diyAudio Member
Join Date: Nov 2009
Location: Toronto
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Quote:
There is no simple relationship between Q and likelyhood of excitation. With a mechanical system, if Q is increased (resistance reduced) then peak height goes up. Area under the curve increases and likelyhood of excitation goes up. The only way to reduce resonant bandwidth while keeping the same resonant frequency would be to increase mass reactance and stiffness reactance in step, hard to do. The fact that peak heights are fairly constant is proof that the resonances are equally likely to be stimulated. David S |
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#18 | |
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frugal-phile(tm)
diyAudio Moderator
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Quote:
dave
__________________
community sites t-linespeakers.org, frugal-horn.com, frugal-phile.com ........ commercial site planet10-HiFi p10-hifi forum here at diyA |
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#19 | |
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diyAudio Member
Join Date: Nov 2009
Location: Toronto
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Quote:
David S |
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#20 |
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diyAudio Member
Join Date: Nov 2009
Location: Toronto
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Here is some more.
http://downloads.bbc.co.uk/rd/pubs/reports/1958-31.pdf Page 20 (25 of the PDF) shows the output of a cabinet with and without a damping layer. Strong sequence of resonances from 200 to 3000 Hz. This was a fully sealed cabinet with a buried internal driver. David S |
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