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Notes on Relativity and Cosmology - Physics Department, UCSB

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34 CHAPTER 1. SPACE, TIME, AND NEWTONIAN PHYSICS<br />

A<br />

V<br />

BA<br />

t<br />

V<br />

CB<br />

t<br />

V<br />

CA<br />

B<br />

t<br />

C<br />

time t<br />

WLOG, take t=0 here<br />

At time t, the separati<strong>on</strong> between A <strong>and</strong> C is V CA t, but we see from the diagram<br />

that it is is also V CB t + V BA t. Canceling the t’s, we have<br />

V CA = V CB + V BA . (1.2)<br />

QED<br />

⋆ ⋆ ⋆ Now, our instructi<strong>on</strong>s about how to draw the diagram (from the facts that<br />

our ideas about time <strong>and</strong> positi<strong>on</strong> are well-defined) came from assumpti<strong>on</strong>s<br />

T <strong>and</strong> S, so the Newt<strong>on</strong>ian formula for the additi<strong>on</strong> of velocities is a logical<br />

c<strong>on</strong>sequence of T <strong>and</strong> S. If this formula does not hold, then at least <strong>on</strong>e of T<br />

<strong>and</strong> S must be false! Of course, I have still not given you any real evidence<br />

to doubt (1.1) – I have <strong>on</strong>ly heavily foreshadowed that this will come. It is a<br />

good idea to start thinking now, based <strong>on</strong> the observati<strong>on</strong>s we have just made,<br />

about how completely any such evidence will make us restructure our noti<strong>on</strong>s<br />

of reality.<br />

• Q: Where have we used T?<br />

• A: In c<strong>on</strong>sidering events at the same time (i.e., at time t <strong>on</strong> the diagram<br />

above).<br />

• Q: Where have we used S?<br />

• A: In implicitly assuming that d BC is same as measured by any<strong>on</strong>e (A,B,<br />

or C).<br />

1.5 Newt<strong>on</strong>’s Laws: Are all reference frames<br />

equal?<br />

The above analysis was true for all reference frames. It made no difference how<br />

the clock that defines the reference frame was moving.

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