Calculating Frame Speed with Relativity and Rocket Events

Read moreIn summary, the conversation discusses two rockets, each with a rest length of 100 meters, and their positions and movements in frame S and S'. Event A and B are mentioned, with B being used to calculate the speed V of S' relative to S. Different equations and methods are used to calculate V, resulting in slightly different answers. The conversation ends with a discussion about possible errors in the calculations.
  • #1
tony873004
Science Advisor
Gold Member
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Relativity -- rocket problems

Homework Statement


Consider two rockets, each of rest length 100 meters. Rocket 1 is at rest in frame S and has its nose at x=0 and its tail at x=+100 meters. Rocket 2 is at rest in frame S’ and has its nose at x’=0 and its tail at x’=
-100 meters.

Now suppose that frame S’ moves with speed V in the x+ direction relative to frame S.

Event A: The nose of Rocket 2 passes the nose of Rocket 1 at time tA = t'A = 0

Event B: The tail of Rocket 2 passes the nose of Rocket 1 at time tB = 2.5 microseconds in frame S.


Use the information about event B to calculate the speed V of S’ relative to S.

Homework Equations



v=d/t

[tex]L = \frac{{L_0 }}{\gamma } = L_0 \sqrt {1 - \frac{{v^2 }}{{c^2 }}} [/tex]

[tex]T = T_0 \gamma = \frac{{T_0 }}{{\sqrt {1 - \frac{{v^2 }}{{c^2 }}} }}[/tex]

The Attempt at a Solution



v=100m / 2.5 microseconds = 40*106 m/s

What doesn't make sense to me is that I used 100 m for d, yet there should be length contraction. So shouldn't I be using a different d? But how do I get that d if I don't know V?
 
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  • #2


tony873004 said:
What doesn't make sense to me is that I used 100 m for d, yet there should be length contraction.
Yes, there should be length contraction.
So shouldn't I be using a different d? But how do I get that d if I don't know V?
You won't be able to get the numerical value of d until you've solved for V, but you can certainly write the length contracted distance in terms of V and thus use it to solve for V.
 
  • #3


Thanks. I'm still confused though.

The length contracted distance in terms of V is

[tex]
L = \frac{{L_0 }}{\gamma } = L_0 \sqrt {1 - \frac{{v^2 }}{{c^2 }}}
[/tex]

and v is
[tex]v = c\sqrt {\left( {1 - \left( {\frac{L}{{L_0 }}} \right)^2 } \right)} [/tex]

So if I substitute the first formula into the 2nd, I get

[tex]
\begin{array}{l}
v = c\sqrt {1 - \,\left( {\frac{{\sqrt {1 - \frac{{v^2 }}{{c^2 }}} }}{{}}} \right)^2 } \,\,\,\, \Rightarrow \,\,\,\,\frac{v}{c} = \sqrt {1 - \,\left( {\sqrt {1 - \frac{{v^2 }}{{c^2 }}} } \right)^2 } \,\,\,\, \Rightarrow \,\,\,\, \\
\\
\,\frac{v}{c} = \sqrt {1 - \,\left( {1 - \frac{{v^2 }}{{c^2 }}} \right)} \,\,\, \Rightarrow \,\,\,\,\,\,\,\left( {\frac{v}{c}} \right)^2 - 1 = - \,\left( {1 - \frac{{v^2 }}{{c^2 }}} \right)\,\,\,\, \Rightarrow \,\,\,\,\,\, \\
\\
\,1 - \left( {\frac{v}{c}} \right)^2 = \,1 - \frac{{v^2 }}{{c^2 }}\,\,\,\, \Rightarrow \,\,\,\,\,\,\,\,\,\,\,\frac{v}{c} = \frac{v}{c} \\
\end{array}
[/tex]
 
  • #4


tony873004 said:
Thanks. I'm still confused though.

The length contracted distance in terms of V is

[tex]
L = \frac{{L_0 }}{\gamma } = L_0 \sqrt {1 - \frac{{v^2 }}{{c^2 }}}
[/tex]

and v is
[tex]v = c\sqrt {\left( {1 - \left( {\frac{L}{{L_0 }}} \right)^2 } \right)} [/tex]

So if I substitute the first formula into the 2nd, I get

[tex]
\begin{array}{l}
v = c\sqrt {1 - \,\left( {\frac{{\sqrt {1 - \frac{{v^2 }}{{c^2 }}} }}{{}}} \right)^2 } \,\,\,\, \Rightarrow \,\,\,\,\frac{v}{c} = \sqrt {1 - \,\left( {\sqrt {1 - \frac{{v^2 }}{{c^2 }}} } \right)^2 } \,\,\,\, \Rightarrow \,\,\,\, \\
\\
\,\frac{v}{c} = \sqrt {1 - \,\left( {1 - \frac{{v^2 }}{{c^2 }}} \right)} \,\,\, \Rightarrow \,\,\,\,\,\,\,\left( {\frac{v}{c}} \right)^2 - 1 = - \,\left( {1 - \frac{{v^2 }}{{c^2 }}} \right)\,\,\,\, \Rightarrow \,\,\,\,\,\, \\
\\
\,1 - \left( {\frac{v}{c}} \right)^2 = \,1 - \frac{{v^2 }}{{c^2 }}\,\,\,\, \Rightarrow \,\,\,\,\,\,\,\,\,\,\,\frac{v}{c} = \frac{v}{c} \\
\end{array}
[/tex]

Your first and second formulas represent the exact same relationship, so its no wonder you're not getting any new information about V. But you actually know two pieces of information here:

(1) The second rocket undergoes length contraction as seen in S:

[tex]L=L_0 \sqrt{1-\frac{V^2}{c^2}}[/tex]

AND

(2) The rocket is moved a distance of [tex]L[/tex] in S, in a time [tex]{\Delta}t=2.5 \mu s[/tex], while traveling at a speed [tex]V[/tex]:

[tex] V=\frac{L}{{\Delta}t}[/tex]
 
  • #5


Thanks. I think I got it. It's more algebra than I though it would be. Can someone double-check that I did this right?

rel1.gif
 
  • #6


tony873004 said:
Thanks. I think I got it. It's more algebra than I though it would be. Can someone double-check that I did this right?

It's correct,although you seemed to be going in circle with your algebra for a little while there...it would have been easier for you to collect the terms that had V^2 on one side of the equation and the rest of it on the other right from the end of your second line of calcs...it probably would have saved you 3 lines or so of algebra.
 
  • #7


You're right. It saved me 3 lines. Thanks!... More relativity q's tommorow...
 
  • #8


New problem...
I get a different answer when I do the algebra the way you recommend.

rel2.gif


I'm recomputing the answers using a more exact value for c:

first method:
sqr(299792458^2*100^2/((2.5e-6)^2*299792458^2+1)) = 39999964.3952457

second method:
sqr((100^2*(299792458)^2) / ((299792458)^2*(2.5e-6)^2+100^2) ) = 39648636.4200608

Assuming the first answer is correct, I can now compute the length of the rocket as viewed from frame S:

100 * sqr(1-39999964.3952457^2 / 299792458^2) = 99.1058843255855

Assuming the second answer is correct,
100 * sqr(1-39648636.4200608^2 / 299792458^2) = 99.1215910501519

In each case, the rocket contracts by about 0.9 meters, but the answers are different enough that it worries me.

And as a check, using these numbers to compute velocity, which was given in the problem as 2.5 microseconds:


First method:
99.1058843255855 / 39999964.3952457 = 2.47764931354201E-06

Second method:
99.1215910501519 / 39648636.4200608 = 0.0000025

I'm guessing that this implies that the 2nd method is correct, since I get back the exact value of the given time. But that would mean that I must have made a mistake in the algebra of the 1st method, although I can't find my error. Usually algebra errors give answers that are way off, not nearly-identical.
 
  • #9


tony873004 said:
First method:
99.1058843255855 / 39999964.3952457 = 2.47764931354201E-06

Second method:
99.1215910501519 / 39648636.4200608 = 0.0000025

I'm guessing that this implies that the 2nd method is correct, since I get back the exact value of the given time. But that would mean that I must have made a mistake in the algebra of the 1st method, although I can't find my error. Usually algebra errors give answers that are way off, not nearly-identical.

There is a slight error on your first calculation; when going from line 7 to line 8, you didn't multiply the 1 in the denominator by (100m)^2...It didn't affect your final answer much though because the first term in the denominator works out to be 1.875 X 10^7 m^2 which is much bigger than the 10^4 m^2 term. This is why it's usually best not to play around too much algebraically, there are more places to make an error.
 
  • #10


Thanks. No matter how many times I stared at that, I just couldn't see it. It's obvious now that you point it out.
 

Related to Calculating Frame Speed with Relativity and Rocket Events

What is the theory of relativity?

The theory of relativity, proposed by Albert Einstein, is a fundamental concept in physics that explains the relationship between space and time and how they are affected by gravity.

How does relativity apply to rocket problems?

Relativity is important in rocket problems because it affects the movement and behavior of objects in a high-speed environment, such as space travel. It helps us understand how time, distance, and mass are affected by motion and gravity.

What is the difference between special relativity and general relativity?

Special relativity deals with the principles of motion and how they are perceived by different observers, while general relativity takes into account the effects of gravity and how it affects the curvature of space-time.

What is time dilation in relativity?

Time dilation is the phenomenon in which time appears to pass at a different rate for objects moving at different speeds. This is a consequence of special relativity and is often experienced by astronauts in space.

How does relativity impact space travel?

Relativity plays a crucial role in space travel as it affects the speed, trajectory, and duration of space journeys. It also helps us understand the concept of time travel and the behavior of objects in a high-gravity environment, such as black holes.

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