While that is true my point was that all of that would not come to play if you put it vertically on a stand as a standard stereo speaker. This speaker was designed to be placed horizontally, the way Amir mesaured it.
Yep, not saying otherwise
While that is true my point was that all of that would not come to play if you put it vertically on a stand as a standard stereo speaker. This speaker was designed to be placed horizontally, the way Amir mesaured it.
To be more specific, the DFT/FFT of the impulse response is the frequency response of magnitude and phase (phase also is important).... that's why I asked @amirm to publish the IR data directly so anyone can analyze it at will... like loading it into REW, ARTA, HolmImpulse etcThe impulse response is, for all practical purposes, the frequency response.
Yes, you are right. I meant the time domain graph of the frequency response. One that looks like a fallen pine tree.The impulse response is, for all practical purposes, the frequency response.
Yep, not saying otherwise
To be more specific, the DFT/FFT of the impulse response is the frequency response of magnitude and phase (phase also is important).... that's why I asked @amirm to publish the IR data directly so anyone can analyze it at will... like loading it into REW, ARTA, HolmImpulse etc
The "normal Klippel," the KA3 analyzer is part of NFS and it can indeed measure many things. I can't show individual drivers since that would involve taking apart the speaker.The "normal" Klippel used for measuring transducers can also measure the impulse response and diaphragm excursions, which I think it's only necessary for engineering purposes.
Not sure if this can also be done with NFS, but it will be great if we can also see the impulse response of woofers and midranges.
Transducers mounted on one enclosure and separating each linked speaker to one binding post will be an issue though.
Offering the full set of preprocessed IR data for a reasonable fee might well be a good compromise for those who want do dig in deeper, IHMO not neccesarily a thing only we seasoned professionals would like to do.In my opinion IR data would not be of interest to us amateurs but only to professional speaker designers, which is leading me to the idea that he would better be offering them for a fee to be able to help cover his costs of speaker testing.
I have not yet figured out how to save an impulse file. I can save it numerically but not as a wave file.To be more specific, the DFT/FFT of the impulse response is the frequency response of magnitude and phase (phase also is important).... that's why I asked @amirm to publish the IR data directly so anyone can analyze it at will... like loading it into REW, ARTA, HolmImpulse etc
Any format is fine with me. Converters (SoX) are available or easily written.I have not yet figured out how to save an impulse file. I can save it numerically but not as a wave file.
Because in your room you would probably be chasing Harman preferred response which would look something like this so you would more be bothered to reduce a peak at 1.5kHz.
View attachment 46216
To be clear, I mean I can export the numbers from a graph, not any kind of sound file.Any format is fine with me. Converters (SoX) are available or easily written.
Also there seems to be a bit of confusion as to how room corrections products work as folks need to understand frequency dependant windowing (FDW). The top end room correction products not only allow you a partial correction let's say up to Schroeder for example, but also allows one to calculate the analysis and correction windows above Schroeder. This allows you to correct for "loudspeaker and room" below Schroeder and just a gentle tone control "direct sound" correction above Schroeder. The number one mistake people make when using room correction products is over correcting the high frequencies.
There may be some mixup here. The blue curve is the "old" Harman room curve from some of their DSP processors, whereas @amirm red curve is indeed the preferred in-room response based on Sean Olive's research. See History of Harman Target Curve.
View attachment 46254
Same results with headphones:
View attachment 46255
And with room correction products:
View attachment 46257
There are several other references to this that I did not include that folks can find in the AES papers.
And the measured in-room response of my constant directivity JBL system:
View attachment 46260
Also there seems to be a bit of confusion as to how room corrections products work as folks need to understand frequency dependant windowing (FDW). The top end room correction products not only allow you a partial correction let's say up to Schroeder for example, but also allows one to calculate the analysis and correction windows above Schroeder. This allows you to correct for "loudspeaker and room" below Schroeder and just a gentle tone control "direct sound" correction above Schroeder. The number one mistake people make when using room correction products is over correcting the high frequencies.
Of course, below Schroeder the room dominates. But that is why we have room eq![]()
Not in the garage where it is. I have to get a microphone in there to measure. And at any rate, the garage is not what was modelled in Devantier paper where the formula came from. Fortunately I have a snapshot of the speaker in my theater. It is heavily smoothed but here it is:Any chance, after yo get some sleep, you can do a simple RTA MMM measurement with REW so it can be compared with predicted in-room response?![]()