Bell Spaceship Paradox: A and B's Viewpoint

In summary, the string between A and B spaceships, which are moving with constant acceleration, will snap from the outside observer C's point of view due to length contraction. This is because the distance between A and B remains constant in C's frame, but the length of the string contracts due to relativity of simultaneity. This can also be interpreted as space elongating for moving objects, causing the string to snap.
  • #1
mananvpanchal
215
0
Hello,

Suppose, A and B spaceships are moving with constant acceleration. There is a string tied to spaceships center to center. A is on left of B and B is on right of A. C is outside observer.

As speed increase, A sees that B going further ahead, and B sees A going further behind. So, from ships PoV, string would be broken.

But, from C's PoV, distance between A and B remains constant.

So, I cannot understand, how string would be broken from C's PoV?

Thanks.
 
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  • #2
From C's PoV the string gets length-contracted. So the (constant) distance between A and B is greater than the (contracting) length of the string. Therefore the string snaps.
 
  • #3
mananvpanchal said:
But, from C's PoV, distance between A and B remains constant.

So, I cannot understand, how string would be broken from C's PoV?
The only way that the length of the moving string could remain constant is if it were being stretched apart. (Consider length contraction.)

This--Bell's Spaceship paradox--has been discussed many, many times here. Do a search to find the relevant threads.
 
  • #4
mananvpanchal said:
Hello,

Suppose, A and B spaceships are moving with constant acceleration. There is a string tied to spaceships center to center. A is on left of B and B is on right of A. C is outside observer.

As speed increase, A sees that B going further ahead, and B sees A going further behind. So, from ships PoV, string would be broken.

But, from C's PoV, distance between A and B remains constant.

So, I cannot understand, how string would be broken from C's PoV?

Thanks.

Here is a very good explanation, complete with detailed math.
 
  • #5
DaleSpam, Doc Al, GAsahi

The A and B starts simultaneously and continue with simultaneous constant acceleration in C's frame. But, not in spaceship's frame. The simultaneous changes of speed in C's frame remains spaceships at constant distance in C's frame. The distance remains equals for all journey even the distance is equal to the distance before journey.

From spaceships' frame, distance between them increased than distance before journey. Because, B starts and changes speed before A in spaceships' frame.

Length contraction cannot applied to only string. It can also apply to the space. If space between ships not contracted than how only string can?
 
  • #6
mananvpanchal said:
DaleSpam, Doc Al, GAsahi

The A and B starts simultaneously and continue with simultaneous constant acceleration in C's frame. But, not in spaceship's frame. The simultaneous changes of speed in C's frame remains spaceships at constant distance in C's frame. The distance remains equals for all journey even the distance is equal to the distance before journey.

From spaceships' frame, distance between them increased than distance before journey. Because, B starts and changes speed before A in spaceships' frame.

It is impossible to understand what you are writing (at least, for me). Did you read the Analysis? Do you realize that there are two different frames (launcher vs. the frame comoving with the two rockets)? Do you realize that relativity of simultaneity plays a big role in solving the problem?

Length contraction cannot applied to only string. It can also apply to the space. If space between ships not contracted than how only string can?

Because, as the problem statement says, IN THE FRAME OF THE LAUNCHER, the rockets accelerate in such a way that they KEEP THE DISTANCE BETWEEN THEM CONSTANT. Whereas the length of the string appears contracted due to Lorentz contraction.
 
  • #7
mananvpanchal said:
Length contraction cannot applied to only string. It can also apply to the space. If space between ships not contracted than how only string can?
Why do you think the space between the ships is not contracted?
 
  • #8
mananvpanchal said:
If space between ships not contracted than how only string can?
The distance between the ships stays constant in the launch frame. But the atoms of the string are contracting in the launch frame. At some point they cannot span the constant distance anymore.

You can replace the string with a chain, and consider the individual chain links as rigid elements, which are all contracting as the chain accelerates:

102oxg6.png
 
  • #9
mananvpanchal said:
The A and B starts simultaneously and continue with simultaneous constant acceleration in C's frame. But, not in spaceship's frame. The simultaneous changes of speed in C's frame remains spaceships at constant distance in C's frame. The distance remains equals for all journey even the distance is equal to the distance before journey.
Yes, I said that.

mananvpanchal said:
Length contraction cannot applied to only string. It can also apply to the space. If space between ships not contracted than how only string can?
I have no idea what you are talking about. What is "space's" rest frame, and what is its length in that frame? To use the length contraction formula you have to have an object with a rest frame and a length in that rest frame. I don't know how you would apply that to "space".
 
  • #10
DaleSpam said:
I have no idea what you are talking about. What is "space's" rest frame, and what is its length in that frame? To use the length contraction formula you have to have an object with a rest frame and a length in that rest frame. I don't know how you would apply that to "space".
Good point. Here's how I interpreted his statement about 'space' contracting: Imagine you have two ships traveling at high speed with respect to another observer (arranged as in the Bell set up, once the acceleration is completed). According to the ship frame, the distance between them is L. According to that other observer, the distance is L/γ.
 
  • #11
Doc Al said:
Good point. Here's how I interpreted his statement about 'space' contracting: Imagine you have two ships traveling at high speed with respect to another observer (arranged as in the Bell set up, once the acceleration is completed). According to the ship frame, the distance between them is L. According to that other observer, the distance is L/γ.
If something happens to "space" then "elongation". Moving objects occupy less space then they do while at rest. This can be interpreted as:

a) Moving object is shorter than at rest (the usual interpretation)
b) Space is elongated for a moving object

Interpretation b) sounds a bit weird. But when you go into a rotating frame, rulers at rest measure a circumference greater than 2πr. You cannot claim that the rulers are contracted, because they are at rest. You must conclude that the space along the circumference is elongated.
 
  • #12
A.T. said:
But when you go into a rotating frame, rulers at rest measure a circumference greater than 2πr. You cannot claim that the rulers are contracted, because they are at rest.
A rotating frame is non inertial so rulers at rest can contract. You cannot simply apply the formulas for inertial frames.
 
  • #13
Doc Al said:
Good point. Here's how I interpreted his statement about 'space' contracting: Imagine you have two ships traveling at high speed with respect to another observer (arranged as in the Bell set up, once the acceleration is completed). According to the ship frame, the distance between them is L. According to that other observer, the distance is L/γ.
Yes, that is reasonable. Then the condition for snapping is that the distance between the ships is greater than the length of the string. In the ships frame that condition is met because the length stays the same and the distance increases. In the launch frame that condition is met because the distance stays the same and the length contracts.
 
  • #14
DaleSpam said:
Yes, that is reasonable. Then the condition for snapping is that the distance between the ships is greater than the length of the string. In the ships frame that condition is met because the length stays the same and the distance increases. In the launch frame that condition is met because the distance stays the same and the length contracts.
Right!
 
  • #15
DaleSpam said:
A rotating frame is non inertial so rulers at rest can contract.
But it is not the length contraction from movement, because they are at rest. It is the apparent contraction that we get, when observing rulers resting further down in a gravitational field from a distance. This is however usually not interpreted as "contraction of the rulers", but rather "distortion of space".
 
  • #16
Ok... Thanks guys.. for detailed explanation.
 
  • #17
I usually recommend <http://arxiv.org/abs/0906.1919> for this.
 
Last edited by a moderator:

1. What is the Bell Spaceship Paradox?

The Bell Spaceship Paradox is a thought experiment proposed by physicist John Bell in 1976. It explores the concept of time dilation and different perceptions of time between two observers in relative motion.

2. Who are A and B in the Bell Spaceship Paradox?

In the Bell Spaceship Paradox, A and B are two observers traveling in separate spaceships at high speeds. They are used to represent two different frames of reference with different perceptions of time.

3. What is the paradox in the Bell Spaceship Paradox?

The paradox arises when A and B observe the same event but have different perceptions of the order of events. This challenges the concept of a universal time and raises questions about the relativity of time.

4. How does the Bell Spaceship Paradox relate to Einstein's theory of relativity?

The Bell Spaceship Paradox is a thought experiment that supports the theory of relativity, specifically the concept of time dilation. It illustrates how time can appear to pass differently for observers in relative motion.

5. What implications does the Bell Spaceship Paradox have in the real world?

The Bell Spaceship Paradox highlights the fundamental principles of relativity and challenges our understanding of time. It has implications in fields such as space travel, where accurate timekeeping is crucial, and in our everyday lives, where our perception of time may be different from others depending on our relative motion.

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