Notes on Relativity and Cosmology - Physics Department, UCSB
Notes on Relativity and Cosmology - Physics Department, UCSB
Notes on Relativity and Cosmology - Physics Department, UCSB
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3.8. HOMEWORK PROBLEMS 79<br />
<strong>on</strong>ce each sec<strong>on</strong>d, how much time passes in your reference frame between<br />
two of it’s ticks?<br />
Hint: Your calculator may not be able to deal effectively with the tiny<br />
numbers involved. As a result, if you just try to type formula (3.3) into<br />
your calculator you may get the value 1. What I want to know is how<br />
much the actual value is different from 1. In cases like this, it is helpful to<br />
use Taylor series expansi<strong>on</strong>s. The expansi<strong>on</strong>s you need to complete this<br />
problem were given in problem (2-2).<br />
3-7. A mu<strong>on</strong> is a particle that has a lifetime of about 10 −6 sec<strong>on</strong>ds. In other<br />
words, when you make a mu<strong>on</strong>, it lives for that l<strong>on</strong>g (as measured in its<br />
own rest frame) <strong>and</strong> then decays (disintegrates) into other particles.<br />
a) The atmosphere is about 30km tall. If a mu<strong>on</strong> is created in the upper<br />
atmosphere moving (straight down) at 1 2c, will it live l<strong>on</strong>g enough to<br />
reach the ground?<br />
b) Suppose that a mu<strong>on</strong> is created at the top of the atmosphere moving<br />
straight down at .999999c. Suppose that you want to catch this mu<strong>on</strong><br />
at the surface <strong>and</strong> shoot it back up at .999999c so that it decays just<br />
when it reaches the top of the atmosphere. How l<strong>on</strong>g should you hold<br />
<strong>on</strong>to the mu<strong>on</strong>?<br />
3-8. For this problem, c<strong>on</strong>sider three inertial observers: You, Alice, <strong>and</strong> Bob.<br />
All three of you meet at <strong>on</strong>e event where your watches all read zero. Alice<br />
recedes from you at 1 2 c <strong>on</strong> your left <strong>and</strong> Bob recedes from you at 1 2 c <strong>on</strong><br />
your right. Draw this situati<strong>on</strong> <strong>on</strong> a spacetime diagram in your frame of<br />
reference. Also draw in a light c<strong>on</strong>e from the event where you all meet.<br />
Recall that you measure distances using your own lines of simultaneity,<br />
<strong>and</strong> note that you find each of the others to be ‘halfway between you <strong>and</strong><br />
the light c<strong>on</strong>e’ al<strong>on</strong>g any of your lines of simultaneity.<br />
Now, use the above observati<strong>on</strong> to draw this situati<strong>on</strong> <strong>on</strong> a spacetime<br />
diagram in Alice’s frame of reference. Use this sec<strong>on</strong>d diagram to estimate<br />
the speed at which Alice finds Bob to be receding from her. What happens<br />
if you draw in another observer (again meeting all of you at t = 0) <strong>and</strong><br />
traveling away from Bob <strong>on</strong> the right at 1 2c as measured in Bob’s frame of<br />
reference??<br />
3-9. C<strong>on</strong>sider a specific versi<strong>on</strong> of the ‘train paradox’ that we discussed in class.<br />
Suppose that we a have tunnel of length 100m (measured in its rest frame)<br />
<strong>and</strong> a train whose length is 100m (measured in its rest frame). The train<br />
is moving al<strong>on</strong>g the track at .8c, <strong>and</strong> the robbers want to trap it using the<br />
following scheme: <strong>on</strong>e robber will sit at the entrance to the tunnel <strong>and</strong><br />
blow it up just after the back end of the train has entered, while the other<br />
robber will sit at the exit of the tunnel <strong>and</strong> blow it up just before the fr<strong>on</strong>t<br />
end of the train gets there.