Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/5/84; site mordor.UUCP Path: utzoo!linus!philabs!cmcl2!seismo!ut-sally!mordor!@S1-A.ARPA:host.MIT-MC.ARPA From: @S1-A.ARPA:host.MIT-MC.ARPA Newsgroups: net.space Subject: Re: Speed Of Light (explain this too) Message-ID: <1768@mordor.UUCP> Date: Sun, 12-May-85 17:03:45 EDT Article-I.D.: mordor.1768 Posted: Sun May 12 17:03:45 1985 Date-Received: Tue, 14-May-85 08:28:56 EDT Sender: daemon@mordor.UUCP Lines: 30 From: Rick McGeer Well, in fact you are observing the objects A and B from a third reference frame with observer, C, and we presume that observers in A, B, and C all have meter sticks, clocks and what have you. From the question we say that in C's reference frame, both A and B are moving in one dimension on opposite vectors with velocity .6 c. The question is, in A's reference frame, what is B's velocity? From Tipler, pg 680, we obtain: u(x') = (u(x) - v)/(1 - v u(x) / c^2) where v is the velocity of A in the frame of C, u(x) is the velocity of B in the frame of C, and u(x') is the velocity of B in the frame of A. Solving for u(x) = -v = -.6c, we get: u(x') = -1.2c/1.36 or almost exactly -.97c. Rick. ps -- the formula I gave above can be obtained by differentiating the Lorentz Transform: x' = gamma (x - vt) where v is the velocity of the frame S' in terms of the frame S. R.