Sonics of Soundlabs


Hello all,

I am contemplating the purchase of a pair of Soundlab M3's, and wonder if some of you guy's (and gals) could help me out a little. They have the newer upgraded transfomers etc. but were manufactured in the late 90's. I am currently using an ARC VT-200 into Martin Logan Prodigy's and love the sound but have always heard great things about the big Soundlabs stats.

For curiousity sake I auditioned a pair of Maggie 3.6's a few weeks ago and they didn't do it for me; there was no bottom end and the dynamics just were not there.......... I thought they did some things well but much preferred the Prodigy's in the end.

I would be buying these speakers used and will not be able to audition fully before purchase. Can anyone tell me how thier sonics compare to my two other "panel" references (the Maggie's and ML's)? Are there any issues (aside from the size) that I should consider when buying a pair of these speakers used? How do the M-3's stack up to the A1's and M1's? Do they match well with the rest of my system..... If I had to find a more powerful amp for instance it would probably be a deal breaker.

Thanks all in advance.

Chris
cmo
Atmasphere -- I believe I did mention that in my post :~)

These principles apply to all loudspeakers, not just Soundlabs. However most loudspeakers can't match both the output and frequency range of products like Soundlabs, Wilsons, etc. etc.
You guys have it backwards concerning room size. Once you get a wavelength that is longer than the room, you get what is termed room gain, on the order of 12db/per octave. (In an actual room it is less due to the walls flexing and losses through the walls, but the gain is there). Smaller rooms = more bass.
Mcreyn -- you are incorrect. When a half wavelength (~ 28 ft for a 20 cycle/sec tone) is longer than the longest dimension of the room, it cannot fully form in space before hitting a wall and reflecting. causing it to double back on itself, producing points of both cancellation and reinforcement. If you happen to be at one of the reinforcing points, it may appear that the bass is very loud, but just a few feet away there may be a null point with very little bass due to cancellation. Right at a wall surface, there is always louder bass because that's where the wave changes direction, therefore releasing a lot of energy when it momentarily stops before being reflected in the opposite direction. That phenomena happens in all rooms though, regardless of size.

If your analysis was correct, then shorter organ pipes would produce lower notes :~)

,
You are speaking about standing waves, which is different than room gain. Room gain results from the maximum length of the wavelength being longer than the room. You do not have standing waves at frequencies below this fundamental frequency, only above. The way to compute the lowest resonant frequency of the room it to take 1127 (or if metric 343) divided by (longest room dimension x2). The result is the lowest freqency that you can have a standing wave and the knee freqeuncy below which you experience room gain.

You analogy of an organ pipe is incorrect as an organ depends on resonance to produce sound. This is far different than sitting in an enclosed area (a room) with a device that puts out an accoustic signal.

Here is a quote from Tom Noussaine on the subject:

"2. Room gain: Room gain starts at roughly the frequency of your lowest axial mode. The pressure gain is 12 dB per octave as frequency falls. In a car its at 60-70 hz depending on size. In my 2136 cubic foot older listening room it started at just below 30 Hz. In my 7500 cubic foot current room it starts at 16 Hz. A Velodyne FSR-15 had 8 dB less output at 2 meters in the larger room with idntical placement."

http://archive.avsforum.com/avs-vb/history/topic/39249-1.html
Mcreyn -- standing waves are only produced when a room dimension is a whole multiple (not a fraction) of the half wavelength of the frequency in question. The room will gain in dB (more SPL than the speaker is putting out) by resonating at the frequency in question (like an organ pipe) and that is why bigger rooms have lower resonant frequencies (per Mr. Noussaine's remarks)

Once again, a room smaller than a certain frequency's half wavelength cannot resonate at that frequency and thus the SPL cannot increase over what the speaker is putting out by itself.

I also read Mr. Noussain's remarks on avht. The smallest room he mentions (assuming an 8 foot ceiling) is quite big enough to develop a full 20 cycle wave (roughly 13x20), and so standing waves (and room gain) are definitely possible at that frequency -- however, in a room too small for the 20 cycle wave to form in the air, standing waves, and therefore room gain are not possible.

As for his weird experience with the Velodyne: A loudspeaker will always put out the same SPL (at a given frequency, at a given power input, at a given distance away from it) in any environment (or even outdoors) at normal atmospheric pressure UNLESS there is either cancellation or reinforcement at the point where the measurement is being taken (which is probably what happened to Mr. Noussaine, and he just didn't realize it.)

I had trouble visualizing how he placed a speaker "identically" in two rooms of different size -- so I'm not sure what the heck he meant; maybe he meant "proportionately" since "identically" would be geometrically impossible. It sounds like he once again stumbled onto a null point without realizing it.

In any case, I would not be especially drawn to his remarks in the future.

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