- Thread Starter
- #81
But the fact that the group delay is around 80 ms at 130 and 170 Hz is a bit worrying. Except if these parts are at the bottom of dips in the amplitude response curve, as it is often the case. Then it doesn't matter, since these frequencies are nearly silent.
They are bottom of dips. Btw, I based my amplitutude correction on MMM RTA pink noise which averaged those narrow dips.
Here is how single sweep looks from LP:
Unsmoothed (I don't know if it is normal that it is so "choppy")
with 1/12 smoothing
But if I take 9 measurements sweeps around my listening sofa and average them you won't be seeing these peaks.
It would look like this (unsmoothed):
What's the sweep size used as a test signal ? For phase and GD measurement from the listening position, I think that the longest one is best (1M). In any case, the length of the test signal has a clear effect on this graph.
I don't know if the fact that the microphone is perfectly still during the measurement matters.
512K. I was holdig mic by hand.
So here, we have the group delay of only a part of the sound : the direct sound and its first reflections (it's completely anechoic only below, say, 1ms, that is only above 1000 Hz in this graph).
It's a bit difficult for me to understand what it means. I can understand what means the amplitude response with Frequency Dependant Window. It's the tonal balance of the attacks in the sound, with reverberations in the room left aside. I can imagine the spectrum changing with time, and being different in the first milliseconds, while we are hearing the direct sound of the speaker, then changing as the sound decays, while we are hearing the sound of the room.
But phase changing as sound decays ?
If I understand correctly, it gives an idea of the time coherence of the attacks that reach our ears before the sound begins to decay in the room.
The two previous peaks, at 130 and 170 Hz, are still visible here, reduced in amplitude. But we can't tell if they come from the direct sound (then it matters, as this represents the time coherence of the speaker) or from the first reflections in the room, that the 12 cycle windowing includes.
In the later case, they should be ignored, as they are just remnants of the peaks in the initial graph, not completely canceled because of the too wide windowing.
I believe those peaks are not coming from direct sound but are caused by first reflections as they vanish when I reduce # of cycles in FDW.
Here it is how it looks with 1/6 cycles, no smoothing:
3cycles:
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