Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!utgpu!water!watmath!clyde!rutgers!ames!sdcsvax!ucbvax!ucbcad!zen!cory.Berkeley.EDU!heppell From: heppell@cory.Berkeley.EDU.UUCP Newsgroups: rec.audio,sci.physics,sci.electronics Subject: Re: Mercury Filled Speaker Wire Message-ID: <3714@zen.berkeley.edu> Date: Sat, 12-Sep-87 18:01:30 EDT Article-I.D.: zen.3714 Posted: Sat Sep 12 18:01:30 1987 Date-Received: Sun, 13-Sep-87 09:04:07 EDT References: <3816@watdcsu.waterloo.edu> <578@uthub.toronto.edu> <3827@watdcsu.waterloo.edu> <14647@topaz.rutgers.edu> Sender: news@zen.berkeley.edu Reply-To: heppell@cory.Berkeley.EDU.UUCP (Kevin G. Heppell) Distribution: rec Organization: University of California, Berkeley Lines: 20 Xref: utgpu rec.audio:2739 sci.physics:2068 sci.electronics:1154 In article <14647@topaz.rutgers.edu> ron@topaz.rutgers.edu (Ron Natalie) writes: > Theoretically, if you had the same resistance, >dialectric, and relative conductor spacings (and shape) you'd get the same >performance regarless of what the conductor was made of. Actually, transmission line performance can vary greatly with conductor resistance. At low frequencies, (low is relative to the transmission line) most of the conduction is bulk instead of surface, but concuctor resistance still matters. The resistance of the conductor affects such things as signal degradation and propagation velocity, which will in turn affect dispersion. Admittedly, between DC and 20 kHz, there is little difference, but some audiophiles will claim to be able to hear it. If there is interest, or I have time, I'll work through the equations and post results. -------------------------------------------------------------------------------- Kevin G. Heppell USNail: 784 Santa Barbara Rd. USENET: ucbvax!cory!heppell Berkeley, CA 94707-2046 arpa: heppell@cory.Berkeley.EDU (415) 528-6396