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Notes on Relativity and Cosmology - Physics Department, UCSB

Notes on Relativity and Cosmology - Physics Department, UCSB

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68 CHAPTER 3. EINSTEIN AND INERTIAL FRAMES<br />

then I must find your stick to be shorter. As a result, c<strong>on</strong>sistency requires both<br />

of us find the two meter sticks to be of the same length.<br />

We c<strong>on</strong>clude that the length of a meter stick is the same in two inertial<br />

frames for the case where the stick points in the directi<strong>on</strong> perpendicular to the<br />

relative moti<strong>on</strong>.<br />

3.5.2 Light Clocks <strong>and</strong> Reference Frames<br />

The property just derived makes it c<strong>on</strong>venient to use such meter sticks to build<br />

clocks. Recall that we have given up most of our beliefs about physics for the<br />

moment, so that in particular we need to think about how to build a reliable<br />

clock. The <strong>on</strong>e thing that we have chosen to build our new framework up<strong>on</strong> is<br />

the c<strong>on</strong>stancy of the speed of light. Therefore, it makes sense to use light to<br />

build our clocks. We will do this by sending light signals out to the end of our<br />

meter stick <strong>and</strong> back. For c<strong>on</strong>venience, let us assume that the meter stick is <strong>on</strong>e<br />

light-sec<strong>on</strong>d l<strong>on</strong>g. This means that it will take the light <strong>on</strong>e sec<strong>on</strong>d to travel<br />

out to the end of the stick <strong>and</strong> then <strong>on</strong>e sec<strong>on</strong>d to come back. A simple model<br />

of such a light clock would be a device in which we put mirrors <strong>on</strong> each end of<br />

the meter stick <strong>and</strong> let a short pulse of light bounce back <strong>and</strong> forth. Each time<br />

the light returns to the first mirror, the clock goes ‘tick’ <strong>and</strong> two sec<strong>on</strong>ds have<br />

passed.<br />

Now, suppose we look at our light clock from the side. Let’s say that the rod in<br />

the clock is oriented in the vertical directi<strong>on</strong>. The path taken by the light looks<br />

like this:<br />

However, what if we look at a light clock carried by our inertial friend who<br />

is moving by at speed v? Suppose that the rod in her clock is also oriented<br />

vertically, with the relative moti<strong>on</strong> in the horiz<strong>on</strong>tal directi<strong>on</strong>. Since the light<br />

goes straight up <strong>and</strong> down in her reference frame, the light pulse moves up <strong>and</strong><br />

forward (<strong>and</strong> then down <strong>and</strong> forward) in our reference frame. In other words,<br />

it follows the path shown below. This should be clear from thinking about the<br />

path you see a basketball follow if some<strong>on</strong>e lifts the basketball above their head<br />

while they are walking past you.

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