https://www.audiosciencereview.com/...ct-spinorama-cea2034-from-the-nfs-data.14141/
???
https://www.audiosciencereview.com/...s/20211124-octave-matlab-ppr-v1-0-zip.167722/
This appears to be the latest and most worked out version.
???
https://www.audiosciencereview.com/...s/20211124-octave-matlab-ppr-v1-0-zip.167722/
This appears to be the latest and most worked out version.
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Tom, searching reading and absorbing is what I do daily. I can usually find things. Except for a few times. Like the original Thesis paper that Klippel based their system on. It is buried. Myself along with the truly smart people ( I'm not anywhere near these guys in my maths proficiency ) on the Audio Science thread tried for a few months to find that original paper. It is scrubbed off of the internet. But we did find a few alternate methods of doing the same thing by students that were not disciples of Herr Klippel. And those were available.
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The spherical harmonics are always real, however each term in the series will be complex owing to the Hankel functions, which are always complex. The fitted coefficients would be complex in the most general case, but maybe real will work?. I investigated this and found that using complex coefficients made the HFs better fit the experimental data. At LFs there was little difference. Low frequencies have few modes in the sum (only one or two in many cases, with one often dominate) so their sensitivity to real versus complex would be much lower.
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The left one is enshrined in the right one making it kind of redundant to add colors. The value of the function is simply how far that point is from the origin (r), and that's apparent from the right hand picture. This confused me when I first saw it (why two?), but then I figured out what I stated above.