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#51 | ||
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diyAudio Member
Join Date: Dec 2002
Location: Planet Earth
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In the electrical/mechanical model, the absorption effects are caused by the lowpass filter.
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We've really gone beyond where the mass-spring model is useful but let's stick with it for a moment. The pics show the frequency response and group delay of 1 ball (blue) and 4 balls (red) with a resonance frequency of 10 KHz. Notice how the F3 moves lower and the group delay (real delay) grows larger at low frequency as you add more balls and a longer spring. If you could build a molecular-size spring-balls gizmo, it might have an F3 for each ball in the GHz range. If you make it very long, say millions of balls, the combined F3 will start to shift down into the audio range and the combined group (real) delay will increase to measurable levels.
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Dennis H |
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#52 |
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diyAudio Member
Join Date: Jul 2005
Location: sydney nsw
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At the time the atomic theory was still doubted by many and the only model of the atom was an ideal perfectly elastic indivisible sphere, first proposed by the Greeks thousands of years before.
I think it was first Boltzmann who pointed out that since they knew that oxygen and nitrogen were diatomic, a more suitable model for them would be a pair of such spheres connected by a rigid rod. This would explain why the speed of sound obtained by Newton was in error, he had considered only single spheres with three degrees of freedom and a diatomic molecule would have five. This also partially explains the effect of water vapour on the speed of sound, the water molecule would have six degrees of freedom, and the speed of sound would vary in accordance with the partial pressures of these three gasses. Later Van der Vaals showed that molecules have a fractional surface charge that causes interactions other than plain momentum preserving perfect impulse collisions. All of this is very interesting but not really relevant for audio since the model of connected elastic spheres en mass acting statistically as waves in a smooth medium is perfectly adequate. rcw. |
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#53 |
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diyAudio Member
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Ok. guys here's directivity plot, 5 deg step, microphone distance 2 meters, 2" midrange driver (STX DT-1300Ti).
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#54 |
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diyAudio Member
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Or smoothed 1/3 octave.
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#55 |
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diyAudio Member
Join Date: Jan 2005
Location: Austria, at a beautiful place right in the heart of the Alps.
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Thanks for your effort to present measurements of the 1m Gaussian MinPhase contour - very much appreciated, Jzagaja !
Have a link to the compression driver used : STX DT-1300Ti ? Michael
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Audio and Loudspeaker Design Guidelines Last edited by mige0; 6th February 2010 at 03:40 PM. |
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#56 |
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diyAudio Member
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STX DT-1300Ti is a driver prototype made for me by STX Soundstation, probably most affordable, high-quality on the market. Smaller brother is here:
D-800-Ti - Sklep internetowy |
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#57 |
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diyAudio Member
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Comparison between JMLC 350Hz (60cm mouth) and Minphase.
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#58 |
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diyAudio Member
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And finally directivity sonogram normalized to axial response.
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#59 |
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diyAudio Member
Join Date: Jan 2005
Location: Austria, at a beautiful place right in the heart of the Alps.
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Where it all started from:
Geddes on Waveguides ![]() ![]() ![]() ![]() Above is not exactly the same Gaussian MinPhase contour thats finally been realized and what we now got measurements for – but might give some background nevertheless ![]() Thanx again, jzagaja - great work ! Michael
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Audio and Loudspeaker Design Guidelines |
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#60 |
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diyAudio Member
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Updated measurements with a good microphone Bruel Kjaer 4149. Directivity 10 deg step, 1/12 oct. smoothing.
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