Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10 5/3/83; site pyuxn.UUCP Path: utzoo!linus!decvax!tektronix!uw-beaver!cornell!vax135!ariel!hou5f!hou5g!hou5h!eagle!mhuxi!mhuxj!mhuxl!mhuxm!pyuxi!pyuxn!rlr From: rlr@pyuxn.UUCP Newsgroups: net.audio Subject: Re: CD principles Message-ID: <259@pyuxn.UUCP> Date: Fri, 30-Sep-83 09:49:51 EDT Article-I.D.: pyuxn.259 Posted: Fri Sep 30 09:49:51 1983 Date-Received: Sun, 2-Oct-83 06:54:01 EDT References: drufl.661 <165@metheus.UUCP> Organization: Bell Labs, Piscataway Lines: 17 I believe that there has been research done that states that one cannot tell the difference between a tone (say a square wave) which has a certain harmonic content (a square wave contains all odd harmonics in amounts inversely proportional to their harmonic number) and another tone with equivalent harmonic content where the phases of some of the harmonic components are reversed in the resulting waveform (which in this case, would no longer be a square wave in shape as a result). It is my understanding that THIS is the kind of phase shift that we are talking about here. This does not imply anything about one speaker producing the square wave and the other producing the altered tone (i.e., phase shift in one of the two speakers but not the other). It implies that if a range of frequencies are shifted uniformly in both speakers, the listener could not distinguish this from the original sound. This was from a course in electronic music and acoustics many years ago, so I don't remember where this is documented.