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#3341 | |
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diyAudio Member
Join Date: Jun 2007
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Quote:
who am I to argue? ![]() just asking because It seemed to me that "the way" is somewhat similar to Yours now I know thank You for response ![]() best, graaf
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"high phooey and hystereo" - Yascha Heifetz |
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#3342 | |
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diyAudio Member
Join Date: Dec 2004
Location: Novi, Michigan
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Quote:
I'm not sure, that comment comes from my basic understanding of line sources etc. In odd dimensions (1, 3 5) the impulse response from a source is compact, while in even dimensions (2, 4) it has a tail. This comes from the basic math. A line source is basically a two dimensional source. (Interesting, this is why gravity waves - 4 dimensions - have to have a tail!) Its easy to see why in the case of a line source (not so easy for gravity!!). At any point in space, the contribution from parts of the source further and further away have to arrive at later and later times. The longer the line, the longer the tail. So even a flat piston has a small tail. However, put this flat piston on a waveguide and it will not have a tail anymore, because it will appear to have been created from a point source. You can shade the line array and elliminate the tail (probably on along a line however), but that takes complex shading (time delays), amplitude shading alone will not do it. There is a lot you can get from the basic physics of a situation. |
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#3343 | |
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diyAudio Member
Join Date: Dec 2004
Location: Novi, Michigan
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Quote:
. There simply is no way that I could make a viable product out of these designs myself. Thats why I have given up. The only Summa's are in homes and I can't give out those names for fairness.The "big guys" have created a situation where a speaker that is not heavily marketed has no chance in the marketplace. This keeps the small intruder out of the picture. Its a very smart move on their part. Devastating for the consumer who wants a real option in the marketplace however. |
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#3344 | |
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Master Burner
Join Date: Dec 2002
Location: San Francisco, California
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www.burningamp.com |
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#3345 | |
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diyAudio Member
Join Date: Apr 2006
Location: Glasgow
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Quote:
... possibly this is off topic. But there is no chance of buying decent waveguides in EU, is there? Ken (ps. not "gravity waves", those are 3D) |
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#3346 |
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diyAudio Member
Join Date: Jun 2005
Location: Lierde
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Here's another candidate for the midbass: the JA8008 HES
Troels Gravesen who you probably know from his excellent website: http://www.troelsgravesen.dk/Diy_Lou...r_Projects.htm has developed a high efficiency driver: the JA8008 HES Specs can be found here: http://jantzen-audio.com/download/PD...Oct07_v1-f.pdf It seems to be an excellent driver according to this enthusiast review from someone who has used the JA8008 HES: http://www.troelsgravesen.dk/JA8008_response.htm Some more info: http://www.troelsgravesen.dk/JA8008.htm |
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#3347 | |
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diyAudio Chief Moderator
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That is why I never recommended a medium format Line Array in a normal venue, where a Nexo Alpha or PS 15 System could do just fine. Nobody ever listened to me against the notion that the all hot Line Array thing was the new Swiss knife. But hey, it looks cooler hanging than stacked, doesn't it? |
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#3348 | |
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diyAudio Member
Join Date: Dec 2004
Location: Novi, Michigan
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Quote:
Actually I didn't discover this. It falls out of the "Green's Function" approach in physics. The Green's Function is basically an impulse response, but unlike an impulse, which is only one dimensional - time - a Green's Function can be defined in any number of dimensions. So my comments came straight out of my "Methods in Theoretical Physics" class at school. I just sent a pair of waveguides to Germany. |
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#3349 | |
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diyAudio Member
Join Date: Jul 2004
Location: Northern Colorado
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Quote:
A drawing of the arrival times on a piece of paper reveals that - nothing more than simple geometry. Multipath is troublesome enough to eliminate from diffraction (and internal cabinet reflections) in conventional speakers (horns or direct-radiators), why multiply the problem with a driver array? At low frequencies (say, below 200 Hz), not much of a problem, since the wavelengths are so much larger than the differential in arrival times. But for frequencies higher than 1 kHz, problems with line arrays in the time, frequency, and spatial domains become much more difficult to resolve. The only two complete solutions have serious drawbacks: 1) A concave curved array will only be accurate at one distance and one lateral bearing angle (one point in space), and badly in error everywhere else. It also bothers me on an esthetic level - concave sound emitters are extremely rare in the natural world, and I would expect a concave emitter to have a weird, hard-to-describe coloration, or perhaps an odd spatial distortion. 2) The Quad ESL63 solution of a phased-array, similar to military radars, has the drawback of simulating the virtual-image point source via multiple delay lines - this requires many amplifiers or a very complex crossover/delay line. Doing so accurately is a process of successive approximation that trades complexity of implementation against accuracy of pulse response - you could get into a million-dollar loudspeaker if you pursued this to the logical conclusion. 3) A partial solution is an amplitude-shaded line array with the outermost radiators sequentially low-passed - which begs the question of the inherent efficiency of the center radiator, which (by definition) sets the efficiency (and headroom) of the whole array. At this point, we are only one step away from a MTM-array multiway loudspeaker system, and two steps away from a traditional MT-array loudspeaker. I think where people go astray is thinking the waves from the individual point-source radiators somehow combine into a cylindrical wavefront - but they don't. They pass right through each other. True, at the very lowest frequencies (comparable to the size of the array), there is mutual coupling and a resulting increase in efficiency, but this falls apart as the wavelengths become shorter. What starts out as an efficient loudspeaker at the lowest frequencies become dominated by comb-filtering and time-dispersal at higher frequencies - and these are errors that are degraded by equalization, since EQ spreads out the time-dispersal even more. Combining high efficiency, ample headroom, and a compact pulse response with rapid time-decay characteristics is a hard nut to crack - the failure of the prosound world to address this over the last sixty years speaks to the scope of the problem. The last serious attempt in the professional world is probably the Shearer theatre horn of 1935 - a long long time ago. The popularity of tap-dancing in movie soundtracks demanded a solution - and I have to admit getting 1 millisecond precision is pretty impressive for 1935. The ingenuity of the Tannoy Dual Concentric deserves an honorable mention as well - impressive technology considering the WWII date of the design. Since then ... well, the soundtracks are (much) louder, and the mass-market-mandated explosions, car crashes, phaser whizzes, and dinosaur thumps come at you from more directions. |
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#3350 | |
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diyAudio Member
Join Date: Aug 2004
Location: Romania
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Quote:
how about the Unity horn? I wouldn't call them point source, but even so it seems they are pretty well regarded for their coherence. And you've mentioned having some 6nd410 midranges. Did you have the chance to listen them? I am asking because I'd like to mate one with a waveguide but I don't know nothing about the subjective performance of these and I am not affording to experiment right now... Good luck with your project! |
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