Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.1 6/24/83; site pur-phy.UUCP Path: utzoo!watmath!clyde!burl!we13!ihnp4!inuxc!pur-ee!CS-Mordred!Pucc-H:Physics:clt From: clt@pur-phy.UUCP (Carrick Talmadge) Newsgroups: net.physics Subject: Re: q.e.d. Q.E.D. Message-ID: <1285@pur-phy.UUCP> Date: Fri, 6-Apr-84 14:32:15 EST Article-I.D.: pur-phy.1285 Posted: Fri Apr 6 14:32:15 1984 Date-Received: Sun, 8-Apr-84 01:29:09 EST References: <1284@pur-phy.UUCP> Organization: Purdue University Physics Dept. Lines: 18 Also, continuing Dwight's defence of Q.E.D., one must distinguish between infinities which arise as a consequence of the field theory, and infinities which arise as a consequence of the method by which we obtain solutions to that field theory (namely via the quantum perturbation method). Infinities may be obtained even in classical field theories, such as General Relativity, when one does a perturbation expansion ( the usual example of this is in solving the two body problem to determine the rate of precession of the perihelion as in the case of the Sun-Mercury system). These infinities are eliminated via "renormalization" just as in the case of a quantum field theory. Carrick Talmadge UUCP: {decvax,ucbvax,harpo,allegra,inuxc,seismo,teklabs}!pur-ee!Physics:clt INTERNET: clt @ pur-phy.UUCP