Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/3/84; site teddy.UUCP Path: utzoo!linus!philabs!cmcl2!seismo!harvard!talcott!panda!teddy!rdp From: rdp@teddy.UUCP Newsgroups: net.audio Subject: Re: RAW SPEAKERS Message-ID: <1042@teddy.UUCP> Date: Mon, 29-Jul-85 12:56:29 EDT Article-I.D.: teddy.1042 Posted: Mon Jul 29 12:56:29 1985 Date-Received: Wed, 31-Jul-85 23:27:13 EDT References: <3177@decwrl.UUCP> <28400013@smu> <1036@teddy.UUCP> Reply-To: rdp@teddy.UUCP (Richard D. Pierce) Organization: GenRad, Inc., Concord, Mass. Lines: 23 In article <1036@teddy.UUCP> rdp@teddy.UUCP (Richard D. Pierce) writes: > >First of all, for a given sound pressure level, the amount of excursion >(displacement) is proportional to the inverse square of the radiating >area, so that at a given frequency, an 8 inch woofer must have a total >excursion TWICE that of a 12 inch woofer. OOOPS, what I meant to say was the amount of excursion is proportional to the inverse square of the DIAMETER of the driver, not the area. But the example I give is correct, as I was computing the areas there. What we are trying to do is maintain a given "volume velocity" for a given sound pressure level so that: Volume Velocity = radiating area x velocity and since the area is proportional to the square of the diameter, the necessary velocity is reduced by the square of the diameter. For a given frequency, the total displacement is proportional to velocity, etc., etc., Sorry... Dick Pierce