Can I get clarification on the constant speed of light

In summary: The implication is that the speed of the light is different depending on the frame of reference you are in.
  • #1
Quandry
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I do not have a problem with the concept of the constant speed of light as it has no mass and therefore no inertia and therefore no relationship to any IFR. However it seems to be expressed as constant in all IFR's which I do not understand. This seems to say that if I am traveling at 1/2c and I shine a torch forward the light moved away from me at c and if I shine the light backwards it also travels away from me at c.
This seems to say that, in the first case, the light is traveling away from the point in space that it is created (independent of my IFR), at 1.5c.
To clarify this for me, my question is:
If I am traveling towards a light source at .5c and I have two light detectors with a set space between them to measure the time that the light takes to transition from one to the other, will the time taken correspond to a speed of c? And, if I decrease my speed to .25c and do the same measurement will the measurement also indicate a speed of c?
 
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  • #2
Quandry said:
This seems to say that, in the first case, the light is traveling away from the point in space that it is created (independent of my IFR), at 1.5c.
No, it's traveling at c in all frames.

 
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  • #3
This is an experimental fact and so is not something you should set out to understand using your regular Galilei transformation. In fact, as you have discovered, it directly violates Galilei addition of velocities. The conclusion you should draw from this is that Galilei addition of velocities does not work in this extreme. Other conclusions such as the relativity of simultaneity follow in a relatively straight forward fashion.
 
  • #4
So you are saying that regardless of my speed, the measurement between to two detectors is always the same?
 
  • #5
Quandry said:
This seems to say that, in the first case, the light is traveling away from the point in space that it is created (independent of my IFR), at 1.5c.
The point in space is a frame-dependent concept. Say your flashlights are on a table on a train. To someone on the train, the point in space where the light was emitted is a point just above the table. To someone standing beside the track, the point in space where the light was emitted is some point above the track where the flashlights happened to be when they emitted.

The emission event is frame-independent, but you can't measure speed with respect to that.
 
  • #6
Orodruin said:
The conclusion you should draw from this is that Galilei addition of velocities does not work in this extreme
I do not set out to understand using Galilei transformation. In fact if you refer to my post I am clear that this does not happen (although it seems a logical, but incorrect, conclusion to the speed of light being a constant in all frames of reference, which by logic says that it is different between two frames of reference). But if I am approaching a source of light which is traveling at c and I am traveling at .5c the relationship between my detector and the source of light is changing at 1.5c, even although the light is traveling at c. There are many incidences where relationships change faster than the speed of light - e.g. phase relationships between traveling waves can move down a waveguide faster than the speed of light.
There is no implication of adding velocities in this process.
 
  • #7
Ibix said:
The point in space is a frame-dependent concept.
It is not the point in space that is frame dependent. It is the observers definition of that point in space relative to other factors.

Ibix said:
The emission event is frame-independent, but you can't measure speed with respect to that
Which I guess is what I am saying - but if you are in the same frame of reference as the photons you can measure speed - but since you are not...
 
  • #8
Quandry said:
...1.5c ...There is no implication of adding velocities in this process.
How did you calculate that 1.5c then?
 
  • #9
Quandry said:
It is not the point in space that is frame dependent. It is the observers definition of that point in space relative to other factors.
How do you define a point without reference to other factors?

Which I guess is what I am saying
An event is a point in spacetime. It doesn't have a velocity for you to compare an object's velocity to.

but if you are in the same frame of reference as the photons you can measure speed - but since you are not...
Light doesn't have a reference frame for you to be in, so measuring speed if you were in it doesn't make sense.
 
  • #10
A.T. said:
How did you calculate that 1.5c then?
I am saying that that is the implication of the light traveling away from me at c, when it is traveling away from the point in space that it was created at c. These two things are incompatible and would require Galilei transformation to make it work.
 
  • #11
Ibix said:
How do you define a point without reference to other factors?
The event happens at a point whether or not you can define it

Ibix said:
An event is a point in spacetime. It doesn't have a velocity for you to compare an object's velocity to.
That is correct, but if the event is defined as the emission of photons you can assume a velocity= c

Ibix said:
Light doesn't have a reference frame for you to be in, so measuring speed if you were in it doesn't make sense.
I guess that's still what I am saying.
 
  • #12
Just going back to my question, it seems that y'all are saying the answer is yes?
Quandry said:
To clarify this for me, my question is:
If I am traveling towards a light source at .5c and I have two light detectors with a set space between them to measure the time that the light takes to transition from one to the other, will the time taken correspond to a speed of c? And, if I decrease my speed to .25c and do the same measurement will the measurement also indicate a speed of c?
 
  • #13
Quandry said:
The event happens at a point whether or not you can define it
An event is a point in spacetime. There will come a time when you say that that event is in the past - it is not in the slice of spacetime you call "now". So you cannot measure a spatial distance to the event "now". You can only decide that some point in "now" is the same as the (spatial part of) the event. That choice is frame dependent - in fact, it's one definition of a choice of frame (up to spatial rotation).

Quandry said:
That is correct, but if the event is defined as the emission of photons you can assume a velocity= c
This is pure nonsense. An event is a point in spacetime. Velocity is the slope of a line in spacetime. A point does not have a slope and there is no way to define one for it. Simply "assuming" an undefined quantity has a particular value is meaningless.

Quandry said:
I guess that's still what I am saying.
Then you are talking nonsense. There is no frame of reference for light - it's a contradiction in terms.
 
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  • #14
Quandry said:
Just going back to my question, it seems that y'all are saying the answer is yes?
Quandry said:
To clarify this for me, my question is:
If I am traveling towards a light source at .5c and I have two light detectors with a set space between them to measure the time that the light takes to transition from one to the other, will the time taken correspond to a speed of c? And, if I decrease my speed to .25c and do the same measurement will the measurement also indicate a speed of c?
Everyone will always measure a time between the reception events consistent with the motion of the detectors (as measured in their frame) and the constant speed of light. Between length contraction, time dilation the relativity of simultaneity, and the different motion of the detectors in any other frame, everyone will always be able to come up with a consistent explanation for why everyone else also comes up with the same invariant speed of light.
 
  • #15
A.T. said:
How did you calculate that 1.5c then?
Quandry said:
I am saying that that is the implication ...
It's a numerical value. How did you calculate it exactly?
 
  • #16
Ibix said:
This is pure nonsense. An event is a point in spacetime. Velocity is the slope of a line in spacetime. A point does not have a slope and there is no way to define one for it. Simply "assuming" an undefined quantity has a particular value is meaningless.
Your response is not relevant. If the event is the result of turning on a torch (as defined) it is reasonable to assume that the event results in photon emission.

Ibix said:
Then you are talking nonsense. There is no frame of reference for light - it's a contradiction in terms.
I m sorry that you think this is nonsense. I was agreeing with you.

'nuff said!
 
  • #17
A.T. said:
It's a numerical value. How did you calculate it exactly?
Exactly? I added 1 and .5 and I got 1.5.

Again, 'nuff said.
 
  • #18
Quandry said:
Exactly? I added 1 and .5 and I got 1.5.

Again, 'nuff said.

That's Galilean relativity! It works only as an approximation in the limit of low speeds.

The correct way is ##\frac{1+0.5}{1+(1)(0.5)}=\frac{1.5}{1.5}=1##.

Google "relativistic velocity addition".
 
  • #19
In addition to what has been said already, one thing that confuses many people is the difference between separation speed and relative speed.

If you are moving to the left with 0.5c relative to an observer A and a light signal travels to the right, then A will see the distance between you and the light growing with 1.5c. This is separation speed.

The above does not mean that you will see the light moving at 1.5c! To draw that conclusion you must assume absolute space and time, which directly contradict SR. In fact, they are basic assumptions behind the Galilei transformation! The basic assumption in SR is that the light will have speed c in your inertial frame too. This is the relative speed.

Also note that there is no way you can objectively say "I am moving at 0.5c" as velocities are relative and change between inertial frames. You need to specify relative to what you move at 0.5c.
 
  • #20
Quandry said:
Your response is not relevant. If the event is the result of turning on a torch (as defined) it is reasonable to assume that the event results in photon emission.I m sorry that you think this is nonsense. I was agreeing with you.
In that case your writing is imprecise, because I'm having trouble reading you as agreeing with me even when you say you are. I think I shall duck out of this conversation for now.
 
  • #21
Quandry said:
There is no implication of adding velocities in this process.
Quandry said:
I added 1 and .5 and I got 1.5.
Hmm...
 
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  • #22
Orodruin said:
If you are moving to the left with 0.5c relative to an observer A and a light signal travels to the right, then A will see the distance between you and the light growing with 1.5c. This is separation speed.
Thanks for the term separation speed. It clarifies the confusion caused by my use of relative speed to mean the same thing.
Can I therefore conclude that, if I am the observer, I see observer A moving right at .5 and, since light belongs to no IFR, I see the same light signal moving to the right and a separation speed between them of .5c
 
  • #23
Quandry said:
Thanks for the term separation speed. It clarifies the confusion caused by my use of relative speed to mean the same thing.
Can I therefore conclude that, if I am the observer, I see observer A moving right at .5 and, since light belongs to no IFR, I see the same light signal moving to the right and a separation speed between them of .5c

Yes, and there's nothing special about light in this specific case. If you see a spaceship approaching from the left at speed ##v### with ##v<c## and another spaceship approaching from the right with speed ##u## (also less than ##c##), you will find that the distance between them is shrinking by ##(u+v)<2c## - that's a separation velocity and it's not the speed of anything in any frame. The right-moving spaceship on the left will consider himself to be at rest while you are moving at speed ##v## and the left-mover is moving at speed ##(u+v)/(1+uv/c^2)## which will always be less than ##c##. Likewise, the left-moving ship on the right will consider himself to be at rest while you are moving at speed ##u## and the right-mover on the left is moving at the same speed ##w##.
 
  • #24
@Quandry welcome to PF Forum,
Perhaps I can help you to understand it.
Quandry said:
I do not have a problem with the concept of the constant speed of light as it has no mass and therefore no inertia and therefore no relationship to any IFR. However it seems to be expressed as constant in all IFR's which I do not understand.

It's hard to quote your questions and answer them at the same time.
So, I'll answer in my own format.
You: This seems to say that if I am traveling at 1/2c and I shine a torch forward the light moved away from me at c and if I shine the light backwards it also travels away from me at c.
You: that if I am traveling at 1/2c.
Answer: With respect to whom? You always have to say in SR that, "I'm traveling at some velocity with respect to something"
So let's just say that you're traveling 1/2c wrt Alice.

You: and I shine a torch forward the light moved away from me at c and if I shine the light backwards it also travels away from me at c.
Answer: Yes!, From your ifr you are at rest. From Alice ifr it's you who is traveling at 1/2c. You are always at rest from your ifr!

You: This seems to say that, in the first case, the light is traveling away from the point in space that it is created (independent of my IFR), at 1.5c.
Answer: No! The light travels at 1c.
You: the light is traveling away from the point in space that it is created (independent of my IFR)
Answer: Yes.
This might be a little confusing. This is where the velocity addition formula comes to mind.
##w = \frac{u+v}{1+uv}##
Let's say you (u) travels at 0.5c and fires a missile 0.4c (v), so from Alice (w) ifr the speed of the missile is
##w = \frac{0.5+0.4}{1+0.5*0.4} = \frac{0.9}{1.2} = 0.75c##
So the speed of the missile in Alice ifr is 0.75c
From yours is (of course) 0.4c
Let's say you (u) travels at 0.5c and shines a light at, of course c or a.
##w = \frac{0.5+1}{1+0.5*1} = \frac{1.5}{1.5} = 1c##
From Alice ifr your light travels at c
from yours, it travels at c.
I see that you already understand that from your responses above.

You: To clarify this for me, my question is:
If I am traveling towards a light source at .5c and I have two light detectors with a set space between them to measure the time that the light takes to transition from one to the other, will the time taken correspond to a speed of c?
Answer: a speed of c? Sure, why not. But it's blue-shifted.
You: And, if I decrease my speed to .25c and do the same measurement will the measurement also indicate a speed of c?
Answer: at a speed of c? Yes, But be careful here, how you do the measurement!

Let's have a detailed thought experiment here.
You (YY) are moving 0.5c to the east, and Alice(AA) from your east is at rest. Y2 is your friend far away from you at east and is comoving with you, that is he travels 0.5c to the east also.
Or Alice will say that it's you who are at rest, and she travels to the west at 0.5c
A2 is Alice friend's who is comoving with her. That is, A2 is traveling to the west at 0.5c
Let's say the distance between YY and Y2 is 1000 light seconds or 300 millions km wrt you!
The distance between A2 and AA is 1000 light seconds wrt you!
Wrt Alice A2 and AA is ##1000/\sqrt{0.75} = 1154.7 \text{ seconds or } 346.4 \text{ millions km}##
But YY and Y2 wrt Alice is ##1000*\sqrt{0.75} = 866.03 \text{ seconds or } 259.8 \text{ millions km}##

Be careful, there will be length contraction and relative simultaneity of event that will come later.
BB is Bob which we will use in later case.
Okay, so here's the picture.

....BB........B2
....YY........Y2
...<------AA........A2

Surely, you will see Alice who is moving toward you at 0.5c to the west and when A2 meets Y2 then A2 shines a light. This light will reach YY 1000 seconds later wrt you, blue shifted. If you don't move 0.25c.
But what if you move 0.25c to the west? There will be two of you here. One who was at rest, and the one who is traveling 0.25c to the west.
So, let's add Bob (BB) who is at rest in your first frame. And now you moves 0.25c to the west wrt Bob. Let's see when YY receives the signal
And let's put B1 at some distance where when YY receives the signal YY will meet B1.
...<---YY.......Y2 ...
......B1...BB.......B3...B2
...<------AA........A2.....

This can be solved by simple algebra.
##0.25T + 1000 = T, T = 1333##
So when YY receives the signal the clock show will 1333. B1 clock not YY clock!
What does YY clock show?
Time dilation.
##\gamma = \frac{1}{\sqrt{1-0.25^2}} = 1.033##
##1333/1.033 = 1291##
YY clock will show 1291 not 1000 not 1333. And the light still travels at c wrt you (YY).
How come that be?
So the only explanation for this situation is this.
Facts that you and Bob both agree
1. When BB meets YY and B2 meets Y2, all of you synchronize your clock.
2. Then A2 meets Y2 and (of course B2) and A2 sends a signal to the west and at that time YY and Y2 moves to the west at 0.25c
3. Now this is tricky. You change frame.
In your new frame, it seems that the light comes further back from Y2.
I think this is rather advanced, although for some people this is very, very bacic. Perhaps you ask about read time dilation, length contraction and relative simultaneity of events.
And the answer about your two detector should come after that. There's a relative simultaneity of events there.

I hope I give the correct answer and the right answer, the answer that you're looking for.
Sincerely
 
  • #25
Stephanus said:
Perhaps I can help you to understand it.
Stephanus, thank you for taking the time to provide such a detailed answer. I was going to say complete, but clearly there is more. However, you have answered my question very well.
Now my challenge is to understand why an observer is required, and why the observer appears to require intelligence.
Thank you for getting me past the barrier,
Bill
 
  • #26
Quandry said:
Now my challenge is to understand why an observer is required, and why the observer appears to require intelligence.
"Observer" usually just means "frame of reference".
 
  • #27
Quandry said:
Now my challenge is to understand why an observer is required
I suggest that you do not, because it is a false statement.
 
  • #28
Quandry said:
Now my challenge is to understand why an observer is required, and why the observer appears to require intelligence.
No observer is required and no intelligence is involved. Putting an observer into the picture is just a convenient way of describing a thought experiment, or of visualizing the origin of a reference frame.
 
  • #29
Quandry said:
Stephanus, thank you for taking the time to provide such a detailed answer. I was going to say complete, but clearly there is more. However, you have answered my question very well.
Now my challenge is to understand why an observer is required, and why the observer appears to require intelligence.
Thank you for getting me past the barrier,
Bill
Hm..., slow down buddy. You are trying to understand SR in an instant. :smile:
A.T. , Orodruin and Nugatory have given you a very good answers about this so called "observer"
 
Last edited:
  • #30
I seem to have a turn of phrase that causes confusion.
I do not say that observers are required, or that intelligence is required. I have seen no explanation which does not use a description of this nature and I wonder how this can be described without observers or intelligence or with just a single IFR (which is a bit of an oxymoron) which is the whole universe.
I am not asking this question in this forum (yet), as I need to understand for myself what this means.
Bill
 
  • #31
Perhaps I can help you...
You are moving 0.1c.
So you are moving from whom? To whom? what?
Can you explain what "you are moving 0.1c" mean?
 
  • #32
Quandry said:
I wonder how this can be described without observers or intelligence
Just replace "observer" with "reference frame", "see" with "is measured in that reference frame" etc.

Quandry said:
or with just a single IFR (which is a bit of an oxymoron) which is the whole universe
In SR there are infinitely many IRFs, and they all contain the whole universe (extend to infinity).
 
  • #33
A.T. said:
In SR there are infinitely many IRFs, and they all contain the whole universe (extend to infinity).

I presume you are referring to Multi Universe, Many Word Interpretation. Not sure that meta-theories should be expressed as assertions, however, I need to come to grips with one universe before tackling infinity.
Many thanks.
 
  • #34
Quandry said:
I presume you are referring to Multi Universe, Many Word Interpretation. Not sure that meta-theories should be expressed as assertions, however, I need to come to grips with one universe before tackling infinity.
Many thanks.
I think not. What A.T. means by many IFRs is not multiverse. They are all in THIS universe. Even though not OBSERVABLE, but they are in THIS universe.
If you travels 100 km / hour to the west, and I travel 100 km/hour to the east. You have your own IFR and I have mine. That's just two of them.
Someone moves 50km/hour to the north would make three.
 
  • #35
OK, I thought he was saying that every IFR contained the whole universe - multiple IFR's means multiple universes. So single universe infinite(?) IFR's is good :)
 

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