Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!mnetor!seismo!rutgers!clyde!cuae2!ihnp4!ihlpa!lew From: lew@ihlpa.UUCP (Lew Mammel, Jr.) Newsgroups: sci.misc Subject: Re: Glass flow Message-ID: <2361@ihlpa.UUCP> Date: Fri, 21-Nov-86 18:02:33 EST Article-I.D.: ihlpa.2361 Posted: Fri Nov 21 18:02:33 1986 Date-Received: Tue, 25-Nov-86 00:05:41 EST References: <17@wjh12.HARVARD.EDU> <666@faron.UUCP> <18@wjh12.HARVARD.EDU> <3786@hplabsb.UUCP> <998@lcuxlm.UUCP> <2372@ecsvax.UUCP> Distribution: net Organization: AT&T Bell Labs, Naperville, IL Lines: 8 A big problem with the thicker-at-the-bottom concept is that the top of the window is still at its original height. If the glass pane is modeled as a viscous flow field, you're going to get tremendous sagging of the top edge. This is not to mention buckling of the plane surfaces. I don't think you can model a free standing glass slab with Euler's equation for viscous flow! Lew Mammel, Jr.