Thanks for posting this thread. Also needs
@mitchco and
@UliBru to weigh in.
I will type out my interpretation of what
@joentell said in this video. The difficulty is that the video is conversational, and I am trying to preserve the meaning in written form. So I can't type out exactly what he said.
- Prior to discussion of his new method of making a target curve, there is a lengthy preamble about target curves, and how it is inappropriate to impose a known "target curve" like the Harman curve on a system. He points out that two different speakers can be equalized to measure the same at the MLP, but they won't sound the same because the major influence is the directivity of the speaker. So far, this seems to be the same point that Dr. Toole made. If you equalize two speakers to measure the same nearfield, they will come a lot closer to sounding the same at the MLP, even if they do not measure the same.
@Floyd Toole has already weighed in
in post #4 of this thread and pointed out that "
a steady-state room curve - which is what is measured at the listening position - is not a “target”, it is a “result".
This is dominated by the off-axis radiation, so a nearfield MMM will not capture it. I have not seen a response from
@joentell yet about this point either in this thread, or in that video.
At 11:40 in the video, there is a description of how a customized target curve for your room is made:
- The difference between a measurement of the speaker's anechoic response, and the MLP measurement of the speaker is the room's transfer function.
- If you make the target the room transfer function, i.e. the delta between the nearfield and the MLP measurement, it will flatten the nearfield response of the speaker.
- You could take a nearfield measurement of the speaker and invert it, and this would flatten the speaker. But this won't correct the bass at the MLP.
- Therefore the best way to correct the bass and flatten the response of the speaker at the same time is to (1) measure the nearfield response of the speaker, (2) measure the response at MLP, (3) subtract nearfield from MLP, and (4) use this as your target (presumably because it will flatten the response of the speaker above Schroder, and correct the bass at the same time).
I would imagine that an alternative approach could work like this:
- take a nearfield MMM of the speaker (ignoring for the time being, Dr. Toole's point above, and assuming for the time being that a nearfield MMM is "good enough" to use as correction). Use this to create an inversion to flatten the response above Schroder.
- take a MMM at the MLP. Use this to flatten the response of low frequencies below Schroder.
- join the two corrections and load that into your convolver
@joentell for the record, I don't feel that you are plugging your product in this thread, nor do I feel that any of your posts are inappropriate or commercial in nature. I find them refreshing and educational. So please continue! This has the potential to become on of the great threads on ASR.
(Note, I am not arguing against anybody here! I can have no opinion of my own, I do not have the qualifications to debate anybody. I only hope that my understanding of the points made is actually the same as the points being made!)