When Will B2 Be Received by A?

In summary, the conversation is discussing the concept of time dilation and the effects of traveling at high speeds on the perception of time. The main question is how the speed of light affects the time it takes for a signal to be received by an observer in a different reference frame. The conversation also touches on the concept of a stationary observer and the potential consequences of an observer traveling at speeds close to the speed of light.
  • #1
Stephanus
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Dear PF Forum,
There's one thing still bothering me.
The speed of light.
Supposed two observer, A and B
A is from the west, B from the east.
Separated by 100 lys.
B sends a signal, say, B1 to A. So B1 will be received by A in 100 years, right?
Now, supposed B travels at 0.8c and at the distance 90lys from A B sends a signal, B2.
B2 will be received by A in 90 years, right?
Not 50 years. I supposed we can't divide 90ly by (c+0.8c), because light travels at (of cource) the speed of light.

And what if 1 second before B sends B2, A suddenly travels at 0.8c?
When will B2 be received by A?
A. 450 years?
Because Va.t + 90ly = c.t
0.8.t+90 = t
t = 450
B. 90 years?
Because A is in the same frame reference of the signal? Or not? Because A travels 1 seconds before the signal was fired.
C. Other?

What if A travels 0.8c the instant B sends B2
When will B2 be received by A?
A. 450 years?
B. 90 years?
C. Other?What if A travels 0.8c 1 second after B sends B2
A. 450 years?
B. 90 years?
C. Other?

What if A travels 0.5c 1 second before B sends B2
A. 270 years? Provided the calculation above.
B. 90 years?
C. Other?

What if A travels 0.5c the instant B sends B2?
What if A travels 0.5c 1 second after B sends B2?

Thanks for any effort to explain to me
 
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  • #2
Stephanus said:
Dear PF Forum,
There's one thing still bothering me.
The speed of light.
Supposed two observer, A and B
A is from the west, B from the east.
Separated by 100 lys. [In which reference frame?]
B sends a signal, say, B1 to A. So B1 will be received by A in 100 years, right?
Now, supposed B travels at 0.8c and at the distance 90lys from A B [In which reference frame?]sends a signal, B2.
B2 will be received by A in 90 years, right?[In which reference frame?]
Not 50 years[In which reference frame?]. I supposed we can't divide 90ly by (c+0.8c), because light travels at (of cource) the speed of light.

And what if 1 second before B sends B2, A suddenly travels at 0.8c[In which reference frame?]?
When will B2 be received by A?[In which reference frame?]
A. 450 years?[In which reference frame?]
Because Va.t + 90ly = c.t
0.8.t+90 = t
t = 450
B. 90 years?[In which reference frame?]
Because A is in the same frame reference of the signal? Or not? Because A travels 1 seconds [In which reference frame?]before the signal was fired.
C. Other?

What if A travels 0.8c [In which reference frame?]the instant B[In which reference frame?] sends B2
When will B2 be received by A[In which reference frame?]?
A. 450 years?[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]What if A travels 0.8c[In which reference frame?] 1 second after B sends B2[In which reference frame?]
A. 450 years?[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]

What if A travels 0.5c 1 second [In which reference frame?]before B sends B2
A. 270 years? Provided the calculation above.[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]

What if A travels 0.5c the instant B sends B2?[In which reference frame?]
What if A travels 0.5c 1 second after B sends B2?[In which reference frame?]

Thanks for any effort to explain to me
 
  • #3
Thanks PeroK for your clarification

Every frame here is in A's frame.

The speed of light.
Supposed two observer, A and B
A is from the west, B from the east.
Separated by 100 lys. [In which reference frame?]
B sends a signal, say, B1 to A. So B1 will be received by A in 100 years, right?
Now, supposed B travels at 0.8c and at the distance 90lys from A B [In which reference frame?]sends a signal, B2.
B2 will be received by A in 90 years, right?[In which reference frame?]
Not 50 years[In which reference frame?]. I supposed we can't divide 90ly by (c+0.8c), because light travels at (of cource) the speed of light.

And what if 1 second before B sends B2, A suddenly travels at 0.8c[In which reference frame?]?
When will B2 be received by A?[In which reference frame?]
A. 450 years?[In which reference frame?]
Because Va.t + 90ly = c.t
0.8.t+90 = t
t = 450
B. 90 years?[In which reference frame?]
Because A is in the same frame reference of the signal? Or not? Because A travels 1 seconds [In which reference frame?]before the signal was fired.
C. Other?

What if A travels 0.8c [In which reference frame?]the instant B[In which reference frame?] sends B2
When will B2 be received by A[In which reference frame?]?
A. 450 years?[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]What if A travels 0.8c[In which reference frame?] 1 second after B sends B2[In which reference frame?]
A. 450 years?[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]

What if A travels 0.5c 1 second [In which reference frame?]before B sends B2
A. 270 years? Provided the calculation above.[In which reference frame?]
B. 90 years?[In which reference frame?]
C. Other?[In which reference frame?]

What if A travels 0.5c the instant B sends B2?[In which reference frame?]
What if A travels 0.5c 1 second after B sends B2?[In which reference frame?]

Thanks for any effort to explain to me
 
  • #4
Stephanus said:
Thanks PeroK for your clarification

Every frame here is in A's frame.

In A's frame the calculation is simple: t = d/c is the time for a light signal to travel a distance d. Regardless of the speed of the light source.

But, A is always stationary in its own reference frame. A cannot travel at 0.8c in its own reference frame. You need to rethink your questions based on that.
 
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  • #5
PeroK said:
In A's frame the calculation is simple: t = d/c is the time for a light signal to travel a distance d. Regardless of the speed of the light source.

But, A is always stationary in its own reference frame. A cannot travel at 0.8c in its own reference frame. You need to rethink your questions based on that.
Wait...
Did you say, any object CAN'T TRAVEL?
So EVERY CALCULATION IN RELATIVIY MUST BE DONE IN THE OBJECT REST FRAME?
EVERYTHING ELSE ARE IN MOTION ACCORDING TO THE OBSERVER?
The observer must think, or destined at rest?
Is that so?
 
  • #6
Stephanus said:
Wait...
Did you say, any object CAN'T TRAVEL?
So EVERY CALCULATION IN RELATIVIY MUST BE DONE IN THE OBJECT REST FRAME?
EVERYTHING ELSE ARE IN MOTION ACCORDING TO THE OBSERVER?
The observer must think, or destined at rest?
Is that so?

There's no way to measure absolute motion. No observer can say "I'm travel absolutely at 100m/s or 0.8c or whatever". All an observer can say is that they are moving with respect to something else.

A can certainly know that initially they were at rest wrt B, then they accelerated and ended up traveling at 0.8c wrt to B. This implies two reference frames: the frame in which A was inititally at rest wrt to B (but now A is traveling at 0.8c) and a new frame in which A is at rest (and B is moving at 0.8c towards A). Measurements of distance and elapsed time will differ in these two frames, so you need to decide which frame of reference you are using.
 
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  • #7
I miss something where. I often see the shorthand "wrt" in the answers of the previous thread.
What is that? With respect to?
 
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  • #8
Stephanus said:
I miss something where. I often see the shorthand "wrt" in the answers of the previous thread.
What is that? With respect to?

Yes!
 
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  • #9
Okay...
Let's say there's a signal coming 90 lys to A and C.
While they are still at rest.
Both synchronize their watches and reset their watches to zero
Then suddenly A travels 0.8 c in the opposite direction of the signal. C keeps staying.
The signal will eventually catches A, right.
What will A watch show when A is receiving the signal?
What will C watch show when C is receiving the signal?
 
  • #10
Stephanus said:
Okay...
Let's say there's a signal coming 90 lys to A and C.
While they are still at rest.
Both synchronize their watches and reset their watches to zero
Then suddenly A travels 0.8 c in the opposite direction of the signal. C keeps staying.
The signal will eventually catches A, right.
What will A watch show when A is receiving the signal?
What will C watch show when C is receiving the signal?

The situation for C is simple: the combined (separation) velocity of A and the light signal is 1.8c. So, it takes 50 years by C's watch for the light to reach A. It's a common misconception that combined (separation) velocities must stay below c, but that is false. C can happily see two objects move with a combined velocity of 1.8c towards each other. And, of course, another 40 years for the light to reach C.

But, A would observe something different. The best way to look at this is to use time dilation (or the Lorentz transformation) to map the time A receives the signal in C's frame (d = 40 lys and t = 50 ys) to A's frame (d' = 0 lys and t' = 30 ys).

You can also use Lorentz to calculate the time and place (according to A) when C receives the signal.

Also, a good exercise is to use Lorentz to calculate where and when the light signal is emitted in A's frame (assuming A is moving at 0.8c towards the signal). It's d = 90 lys and t = 0 in C's frame.
 
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  • #11
Stephanus said:
Then suddenly A travels 0.8 c in the opposite direction of the signal. C keeps staying.
PeroK said:
The situation for C is simple: the combined (separation) velocity of A and the light signal is 1.8c.
Ahh, I must have typed incorrectly. A travels 0.8 at the SAME direction of the signal.
I'm sorry PeroK for your inconvenience.
And thanks for answering me.
 
  • #12
Stephanus said:
Ahh, I must have typed incorrectly. A travels 0.8 at the SAME direction of the signal.
I'm sorry PeroK for your inconvenience.
And thanks for answering me.

The numbers are different, but the principle is the same. Solve in C's frame, then transform to A's frame using Lorentz.
 
  • #13
Sorry to ask the wrong question.
Let's say there's a signal coming 90 lys to A and C.
While they are still at rest.
Both synchronize their watches and reset their watches to zero
Then suddenly A travels 0.8 c in the SAME direction of the signal. C keeps staying.
The signal will eventually catches A, right.
What will A watch show when A is receiving the signal?
What will C watch show when C is receiving the signal?
 
  • #14
Stephanus said:
Sorry to ask the wrong question.
Let's say there's a signal coming 90 lys to A and C.
While they are still at rest.
Both synchronize their watches and reset their watches to zero
Then suddenly A travels 0.8 c in the SAME direction of the signal. C keeps staying.
The signal will eventually catches A, right.
What will A watch show when A is receiving the signal?
What will C watch show when C is receiving the signal?

You do all the calculations in C's frame and then use Lorentz to transform to A's frame. If you didn't understand what I did above, then what's the point of me giving you numerical answers for a new problem if you won't understand those either?
 
  • #15
PeroK said:
You do all the calculations in C's frame and then use Lorentz to transform to A's frame. If you didn't understand what I did above, then what's the point of me giving you numerical answers for a new problem if you won't understand those either?
No, I didn't :smile:
I just understand ##\gamma## in Lorentz Transformation. I'm reading Lorentz Transformation with matrix, now.
Still thanks for the answer.
 
  • #16
It's just that we (the layman) often hears twins paradox, time machine, etc...
At first I think understanding twins paradox is not that hard. But it's very difficult (for me).
Not given up yet.
 
  • #17
PeroK said:
But, A would observe something different. The best way to look at this is to use time dilation (or the Lorentz transformation) to map the time A receives the signal in C's frame (d = 40 lys and t = 50 ys) to A's frame (d' = 0 lys and t' = 30 ys).
Why 30 years?
Is it because ##\gamma = \frac{1}{\sqrt{1-0.8^2}} = \frac{5}{3}##
And ##\frac{50}{\frac{5}{3}}## = 30?
 
  • #18
Stephanus said:
Why 30 years?
Is it because ##\gamma = \frac{1}{\sqrt{1-0.8^2}} = \frac{5}{3}##
And ##\frac{50}{\frac{5}{3}}## = 30?

Yes, that's time dilation, which is a special case of the Lorentz Transformation where you are following A. I.e. in C's reference frame, A's watch is moving, hence time dilated. So, when the light reaches A (in the first problem that's simply after 50 years), A's watch will read (3/5)*50 = 30 yrs.

But, the general Lorentz Transform is:

##t' = \gamma (t - \frac{Vx}{c^2})##

##x' = \gamma (x - Vt)##

So, for events that take place at points other than where A is, you don't have simply time dilation. It's more complicated.

It depends what you are trying to learn with this. To understand Special Relativity you do have to study it thoroughly.
 
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  • #19
PeroK said:
Yes, that's time dilation, which is a special case of the Lorentz Transformation where you are following A. I.e. in C's reference frame, A's watch is moving, hence time dilated. So, when the light reaches A (in the first problem that's simply after 50 years), A's watch will read (3/5)*50 = 30 yrs.

But, the general Lorentz Transform is:

##t' = \gamma (t - \frac{Vx}{c^2})##

##x' = \gamma (x - Vt)##

So, for events that take place at points other than where A is, you don't have simply time dilation. It's more complicated.

It depends what you are trying to learn with this. To understand Special Relativity you do have to study it thoroughly.

And as I read from this
http://en.wikipedia.org/wiki/Lorentz_transformation#Boost_in_the_x-direction
There are still y' and z' that you don't write. But thank you very much. Yours is more to the point! Easier to understand.
 
  • #20
Stephanus said:
Wait...
Did you say, any object CAN'T TRAVEL?
So EVERY CALCULATION IN RELATIVIY MUST BE DONE IN THE OBJECT REST FRAME?
EVERYTHING ELSE ARE IN MOTION ACCORDING TO THE OBSERVER?
The observer must think, or destined at rest?
Is that so?
No, you can calculate anything with a single reference system in which some things are moving, and often (but not always) that is also the easiest. In fact that is what you do when you talk about an object that moves at 0.8c.

If you use a standard reference system for the physics, then this implies that you assume for objects that are not moving relatively to this system, that they are physically in rest (the objects cannot be thought to be in rest and travel at 0.8c). Consequently, from that perspective you assume that:
- the speed of light relative to them is c in all directions
- they are not length contracted
- if they are clocks then they run at normal speed.
 
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FAQ: When Will B2 Be Received by A?

What is the speed of light?

The speed of light is a fundamental physical constant that represents the speed at which light travels through a vacuum. It is approximately 299,792,458 meters per second.

How was the speed of light first measured?

The first successful measurement of the speed of light was conducted by Danish astronomer Ole Rømer in 1676. He observed the variations in the orbital period of Jupiter's moon Io and used this data to calculate the speed of light.

Can anything travel faster than the speed of light?

According to Albert Einstein's theory of relativity, nothing can travel faster than the speed of light. As an object approaches the speed of light, its mass increases and it requires an infinite amount of energy to accelerate it any further.

How does the speed of light affect time and space?

One of the most significant implications of the speed of light is that it sets the cosmic speed limit. This means that nothing can travel faster than the speed of light and time and space are affected by this limitation. As an object approaches the speed of light, time slows down and space contracts.

Why is the speed of light important in science?

The speed of light plays a crucial role in many areas of science, including physics, astronomy, and communications. It is used to measure distances in space, understand the behavior of particles, and develop technologies such as fiber optics for high-speed data transmission.

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