Perceiving Time and Speed at Near Light Speed

In summary: Uh ... I guess I was misled my the words "there is no way to prove that you are the one who is at rest".It corresponds to the way the PoR was originally formulated, and Einstein's formulation of the PoR is perhaps more neutral.I agree that the earlier formulation may suggest a certain interpretation, but not emphatically: in SR any standard reference system pretends to be a "rest system" so that other systems are pretended to be "moving", with all implied physical consequences such as relativity of clock synchronization. To get back to my earlier example, in GPS calculations the speed of light is not isotropic relative to you - because you are held to be...moving.
  • #1
TimeRip496
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5
Two spaceships pass by each other. Both are traveling at near the speed of light. How will each spaceship percieve each other speed and time? Besides how do you do it mathematically?
 
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  • #2
TimeRip496 said:
Two spaceships pass by each other. Both are traveling at near the speed of light. How will each spaceship percieve each other speed and time? Besides how do you do it mathematically?
"Traveling at near the speed of light" is an utterly meaningless statement since you gave no reference frame. YOU are traveling at near the speed of light right this very minute.

If you say there is an observer on Earth and he "sees" one ship approaching at near c and another ship approaching at near c from the opposite direction all in his frame of reference, then the the spaceship captains each see themselves as stationary and the Earth approaching them at close to c and the other spaceship approaching at even closer to c.

Look up Lorentz Transform.
 
  • #3
You might also want to check out the relativistic velocity addition formula. You can derive it from the Lorentz transforms, but it's a direct answer to one of your questions.
 
  • #4
Ibix said:
You might also want to check out the relativistic velocity addition formula. You can derive it from the Lorentz transforms, but it's a direct answer to one of your questions.
Thanks for adding this. I should have mentioned it.
 
  • #5
Well, if you are on the spaceship you can simply say that you are the one at rest and the other ship is going at some speed near ##c##, (of course there is no way to prove that you are the one who is at rest). You will also see the ship to be time-dilated by the standard formula for time dilation. If you are an observer outside both spaceships and you measure both the spaceships' speeds relative to you, and you wanted to know what speed an observer on one spaceship would measure the other going, you use the relativistic velocity addition formula, as Ibix mentioned. The equation is ##w={\frac{u+v}{1+{\frac{uv}{c^{2}}}}}## , ##w## is the combined speed the observer would measure, ##u## is the speed of one ship, ##v## is the speed of the second ship. By knowing what speed an observer on the ship would measure of the other ship, you can then plug ##w## into the formula for time dilation and find out how that observer would measure time being dilated.
 
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  • #6
Physicist97 said:
Well, if you are on the spaceship you can simply say that you are the one at rest and the other ship is going at some speed near ##c##, (of course there is no way to prove that you are the one who is at rest).
There is absolutely no need to "prove" you are at rest in your own frame of reference, you are by definition at rest. And since no one is EVER at rest in any absolute sense, that's the best you can do.
 
  • #7
phinds said:
There is absolutely no need to "prove" you are at rest in your own frame of reference, you are by definition at rest. [..].
For sure, nobody suggests here that one needs to "prove" that you are at rest in "your own frame of reference". And you are for example by definition not at rest but moving in the ECI frame which we use for GPS.
 
  • #8
harrylin said:
For sure, nobody suggests here that one needs to "prove" that you are at rest in "your own frame of reference". And you are for example by definition not at rest but moving in the ECI frame which we use for GPS.
Uh ... I guess I was misled my the words "there is no way to prove that you are the one who is at rest".
 
  • #9
phinds said:
Uh ... I guess I was misled my the words "there is no way to prove that you are the one who is at rest".
That's just one way of stating the PoR. :smile:
 
  • #10
harrylin said:
That's just one way of stating the PoR. :smile:
Well, to me it emphatically suggests a belief that SOMEONE is absolutely at rest, you just can't prove you are that one.
 
  • #11
phinds said:
Well, to me it emphatically suggests a belief that SOMEONE is absolutely at rest, you just can't prove you are that one.
It corresponds to the way the PoR was originally formulated, and Einstein's formulation of the PoR is perhaps more neutral.

I agree that the earlier formulation may suggest a certain interpretation, but not emphatically: in SR any standard reference system pretends to be a "rest system" so that other systems are pretended to be "moving", with all implied physical consequences such as relativity of clock synchronization. To get back to my earlier example, in GPS calculations the speed of light is not isotropic relative to you - because you are held to be moving.
 
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  • #12
harrylin said:
It corresponds to the way the PoR was originally formulated, and Einstein's formulation of the PoR is perhaps more neutral.

I agree that the earlier formulation may suggest a certain interpretation, but not emphatically: in SR any standard reference system pretends to be a "rest system" so that other systems are pretended to be "moving", with all implied physical consequences such as relativity of clock synchronization. To get back to my earlier example, in GPS calculations the speed of light is not isotropic relative to you - because you are held to be moving.
I'm not getting how any of this is relevant to either the original question or the side issue brought up by my response to physicist97
 
  • #13
phinds said:
I'm not getting how any of this is relevant to either the original question or the side issue brought up by my response to physicist97
The side issue that you brought up has probably nothing to do with the original question. I'll therefore end my clarifications as follows: "there is no way to prove that you are the one who is at rest" corresponds to statements like "there is no way to prove that your clock synchronization is right".
 

1. How does time perception change at near light speed?

At near light speed, time dilation occurs, meaning that time appears to move slower for an observer on a fast-moving object compared to an observer at rest. This is due to the theory of relativity, which states that time and space are relative to the observer's frame of reference.

2. Can humans accurately perceive time at near light speed?

No, humans cannot accurately perceive time at near light speed. As an object approaches the speed of light, time appears to slow down to the point where it can seem to stand still. This makes it nearly impossible for humans to accurately perceive time at such high speeds.

3. How does speed affect the perception of time?

The faster an object moves, the slower time appears to pass for that object. This is because as an object approaches the speed of light, its mass increases, and it requires more energy to continue accelerating. This results in time appearing to slow down for the object, as observed by an outside observer.

4. Is there a limit to how fast we can perceive time?

According to the theory of relativity, there is no limit to how fast an object can perceive time. However, as an object approaches the speed of light, time appears to slow down to the point where it can seem to stand still. This makes it nearly impossible for us to perceive time at near light speed.

5. How does the perception of speed change at near light speed?

At near light speed, objects appear to shrink in the direction of motion. This is known as length contraction and is a consequence of time dilation. This means that an object moving at near light speed will appear shorter to an outside observer than it does to someone on the object itself.

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