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Notes on Relativity and Cosmology - Physics Department, UCSB

Notes on Relativity and Cosmology - Physics Department, UCSB

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178 CHAPTER 7. RELATIVITY AND THE GRAVITATIONAL FIELD<br />

The answer of course is the frame that acts like an inertial frame. In this<br />

case, this is the freely falling reference frame. We have learned that, in such a<br />

reference frame, we can ignore gravity completely.<br />

Now, how much sense does the above picture really make? Let’s make this easy,<br />

<strong>and</strong> suppose that the earth were really big.... it turns out that, in this case,<br />

the earth’s gravitati<strong>on</strong>al field would be nearly c<strong>on</strong>stant, <strong>and</strong> would weaken <strong>on</strong>ly<br />

very slowly as we go upward. Does this mesh with the diagram above?<br />

Not really..... We said that the diagram above is effectively in an inertial frame.<br />

However, in this case we know that, if the distance between the bottom <strong>and</strong><br />

top of the tower does not change, then the bottom must accelerate at a faster<br />

rate than the top does! But we just said that we want to c<strong>on</strong>sider a c<strong>on</strong>stant<br />

gravitati<strong>on</strong>al field! So, what’s up?<br />

Side note: No, it does not help to point out that the real earth’s gravitati<strong>on</strong>al<br />

field is not c<strong>on</strong>stant. The point here is that the earth’s gravitati<strong>on</strong>al field<br />

changes in a way that has nothing to do with the relati<strong>on</strong>ship α = c 2 /l from<br />

the accelerated rocket.<br />

7.3.2 How Local?<br />

Well, we do have a way out of this: We realized before that the idea of freely<br />

falling frames being like inertial frames was not universally true. After all, freely<br />

falling objects <strong>on</strong> opposite side of the earth do accelerate towards each other.<br />

In c<strong>on</strong>trast, any two inertial objects experience zero relative accelerati<strong>on</strong>.<br />

However, we did say that inertial <strong>and</strong> freely falling frames are the same ‘locally.’<br />

Let’s take a minute to refine that statement.<br />

How local is local? Well, this is much like the questi<strong>on</strong> of “when is a velocity<br />

small compared to the speed of light?” What we found before was that Newt<strong>on</strong>ian<br />

physics held true in the limit of small velocities. In the same way, our<br />

statement that inertial frames <strong>and</strong> freely-falling frames are similar is supposed<br />

to be true in the sense of a limit. This comparis<strong>on</strong> becomes more <strong>and</strong> more<br />

valid the smaller a regi<strong>on</strong> of spacetime we use to compare the two.<br />

Nevertheless, it is still meaningful to ask how accurate this comparis<strong>on</strong> is. In<br />

other words, we will need to know exactly which things agree in the above limit.

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