source file: mills2.txt Date: Fri, 4 Jul 1997 21:46:56 +0200 Subject: Octave equivalence From: DFinnamore@aol.com In digest #1119 I wrote: > Have you never seen pictures of > waveforms? E.g., given two waves, one of which has a frequency at a > power-of-two of the other, the lower one will cross the zero point (volage- > or SPL-wise) only at points at which the higher one is crossing as well. > This is a unique property of frequencies related by powers-of-two; they > have, then a special relationship of some kind, no? The higher one is > repeating at the same frequency as the lower one, as well as at its own > nominal frequency. They can, then, in a very real and physical sense, be > considered to be the same note; i.e., the same "pitch" but in different > registers. I was wrong. 8-)> Graham Breed was gracious enough to point out my error to me off-list. The above definition would apply to any whole-number multiple of the lower frequency, not just powers of two. However, there is still a unique relationship if you consider that the lower one will cross the zero point only at points at which the higher one is also crossing _and completing an even number of cycles_. It turns out that odd-number multiples cross in mid-cycle where the lower one crosses, and even ones cross at completed cycles. I acknowlege that this weakens my argument considerably. Much more interesting was Marion's observation: >On octave invariance, it has just occurred to me that, in LCM >terms, the octave has a property that no other ratio shares. >That is two notes that differ only by octaves can be mixed >without making the length of the resulting "interference" pattern >longer than the waveform of the lowest note. That's what I was picturing in my mind but stated rather poorly, using the wrong point of reference. Thanks, Marion. So for now I still maintain my conclusion that two pitches separated by the interval 2:1 are the same note in different registers. That triad inversions sound different is the result of a different set of intervals within each inversion of the chord, and so does not seem to require throwing out the idea of octave equivalence. As to Gary M.'s comment that this argument would be distroyed by simply mistuning the octaves slightly, I think that since its proximity to 2:1 causes the ear to treat it (musically) as if it were exactly 2:1, the theory is still valid. David Received: from ns.ezh.nl [137.174.112.59] by vbv40.ezh.nl with SMTP-OpenVMS via TCP/IP; Fri, 4 Jul 1997 22:36 +0200 Received: by ns.ezh.nl; (5.65v3.2/1.3/10May95) id AA23054; Fri, 4 Jul 1997 22:36:44 +0200 Date: Fri, 4 Jul 1997 22:36:44 +0200 Received: from ella.mills.edu by ns (smtpxd); id XA05115 Received: (qmail 11467 invoked from network); 4 Jul 1997 20:36:38 -0000 Received: from localhost (HELO ella.mills.edu) (127.0.0.1) by localhost with SMTP; 4 Jul 1997 20:36:38 -0000 Message-Id: <199707042031.PAA29119@kimserv> Errors-To: madole@mills.edu Reply-To: tuning@eartha.mills.edu Originator: tuning@eartha.mills.edu Sender: tuning@eartha.mills.edu