Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!mnetor!seismo!columbia!rutgers!husc6!mit-eddie!genrad!decvax!mcnc!ecsvax!hes From: hes@ecsvax.UUCP (Henry Schaffer) Newsgroups: sci.physics Subject: Re: A Question Message-ID: <2182@ecsvax.UUCP> Date: Sun, 26-Oct-86 22:06:24 EST Article-I.D.: ecsvax.2182 Posted: Sun Oct 26 22:06:24 1986 Date-Received: Mon, 27-Oct-86 22:29:26 EST References: <230@sri-arpa.ARPA> <572@epimass.UUCP> Organization: NC State Univ. Lines: 29 > In article <230@sri-arpa.ARPA> JDM%SMVL%rca.com@CSNET-RELAY.ARPA writes: ... > o Given the old "accellerating-elevator-in-space" experiment, > how can one within the elevator tell the whether he is > accellerating or under the influence of gravity? > > You can't tell the difference. This is the heart of general > relativity. > > > -- > - Joe Buck {hplabs,ihnp4}!oliveb!epimass!jbuck > Entropic Processing, Inc., Cupertino, California I've wondered about one "difference" which I once read about. Hold a ball in each hand, say 1 meter apart, and level with the floor. Then let go of them, and they will "drop" to the floor - mark where they hit. In the accelerating-at-1g-elevator-in-space they will hit exactly the same distance apart. On the 1-g-surface-of-earth they will be slightly closer together because they fall along radii converging at the center of mass of the earth. What is the loophole here? Can gravity produce parallel paths of the falling balls, or does the elevator test only allow one ball, or ... ? (Please help - I'd hate to discard general relativity because of this. :-) --henry schaffer n c state univ (not physics dept)