Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/18/84; site brl-tgr.ARPA Path: utzoo!linus!philabs!cmcl2!seismo!brl-tgr!gwyn From: gwyn@brl-tgr.ARPA (Doug Gwyn ) Newsgroups: net.physics Subject: Re: Mach's Principle Message-ID: <7855@brl-tgr.ARPA> Date: Wed, 30-Jan-85 12:12:50 EST Article-I.D.: brl-tgr.7855 Posted: Wed Jan 30 12:12:50 1985 Date-Received: Sun, 3-Feb-85 01:50:45 EST References: <4794@ukc.UUCP> Distribution: net Organization: Ballistic Research Lab Lines: 15 Xref: seismo net.physics:2431 Mach's principle was that it should be possible to describe the "forces" on a rotating body in either of two ways, the more interesting of which is to conside the body at rest and the forces as due to the rotation of the rest of the universe w.r.t. the body. Einstein started out a firm believer in Mach's principle but rather lost interest in it (perhaps because it was difficult to show how the effect could be explained in general-relativistic terms). There is no "instantaneous action at a distance" involved, though. Remember that gravitational effects propagate via a field at the speed of light. In all such field theories one has to allow that the field itself can play an active role (e.g. the energy of a solenoid is in its field, which does not "instantaneously collapse" when the current is interrupted).