Two lightnings that happen at the same time, a train and a passanger

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Discussion Overview

The discussion revolves around the concept of simultaneity in the context of special relativity, particularly focusing on a thought experiment involving two lightning strikes observed from different frames of reference: an outside observer and an observer on a moving train. Participants explore the implications of these observations on the nature of light speed and simultaneity.

Discussion Character

  • Exploratory
  • Debate/contested
  • Mathematical reasoning
  • Conceptual clarification

Main Points Raised

  • Some participants note that the observer on the train measures light from point B reaching him before light from point A, suggesting that simultaneity is frame dependent.
  • Others argue that this apparent discrepancy raises confusion about the constancy of the speed of light, questioning if it is merely an excuse to uphold that c is always constant.
  • A participant expresses confusion about how events can be frame independent while simultaneity is frame dependent, suggesting that events occur in only one way.
  • Some participants discuss mathematical transformations related to the Lorentz factor and time dilation, seeking clarification on the derivation of equations related to special relativity.
  • There is a mention of a simpler example involving light in a train to illustrate the relativity of simultaneity, contrasting perspectives from different observers.
  • One participant raises a hypothetical scenario about Earth catching up to a spaceship moving at 0.6c, questioning the implications for aging and time perception between the two frames.
  • Another participant emphasizes that the separation of events in spacetime is dependent on the observer's frame of reference, while asserting that physical phenomena are independent of coordinate systems.

Areas of Agreement / Disagreement

Participants express varying degrees of confusion and disagreement regarding the implications of simultaneity and the constancy of the speed of light. There is no consensus on the interpretation of these concepts, and multiple competing views remain throughout the discussion.

Contextual Notes

Some participants highlight limitations in understanding the implications of simultaneity and the mathematical transformations involved, indicating that assumptions about the nature of light and time may not be fully resolved.

Nikitin
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allright, I'm finishing up my final Gymnasium physics course and the weirdest chapters (QM and Einstein) are at the end.

So here is a book-example I don't understand:

Lightning strikes at point A and B at the same time (if an outside observer is watching). Between A and B is a train moving at a constant speed in the direction AB. An observer M is sitting right in the middle of the train, ie right in the middle of A and B.

The observer measures that he light coming from B reaches him before the light from A.

OK this is weird. I thought that that speed of light is always c to whoever the observer is. So since the light from A and B is approaching the dude at the same speed, shouldn't the light from A & B reach him at the same time?

If the observer sees the light from B first, this would mean that the observer's relative speed to the light from B is > C.
 
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Nikitin said:
The observer measures that he light coming from B reaches him before the light from A.
Note: Everyone (even the outside observer) agrees that light reaches M at different times.
OK this is weird. I thought that that speed of light is always c to whoever the observer is. So since the light from A and B is approaching the dude at the same speed, shouldn't the light from A & B reach him at the same time?
Only if the light starts out at the same time, which is the point. According to the train observers, the lightning strikes were not at the same time. Simultaneity is frame dependent.
 
What? Really? I am so confused, why? Is this just some excuse used to claim that c is always constant?
 
also can you help me with some math? how do I turn t02(1 - c2/v2) to the lorentz factor? I don't know how to convert (1 - c2/v2)-1 into (1 - v2/c2)
 
Nikitin said:
What? obviously the light starts out at the same time..?? how can this be possible lol
The lightning strikes at the same time according to the outside observer on the tracks. But if we assume that light travels at the same speed in every frame, train observers are forced to concluded that the lightning struck B before it struck A.
 
so this is just an excuse to say that c is always constant?

well we know how that cern thing went...
 
Nikitin said:
so this is just an excuse to say that c is always constant?
No, it's a consequence of c being invariant. (And overwhelmingly supported experimentally.)
well we know how that cern thing went...
I assume you're joking.
 
OK, can you help me with post #4?

thanks for ur patience btw, I really appreciate the help
 
Nikitin said:
also can you help me with some math? how do I turn t02(1 - c2/v2) to the lorentz factor? I don't know how to convert (1 - c2/v2)-1 into (1 - v2/c2)
Where is this coming from?

In any case:

(1 - c2/v2) = - (c2/v2)(1 - v2/c2)
 
  • #10
well the book says

2) t2 = c2t02/(c2-v2)

==> 3) t = t0/sqrt(1 - v2/c2)

I don't get how they went from 2 to 3
 
  • #11
Nikitin said:
well the book says

2) t2 = c2t02/(c2-v2)

==> 3) t = t0/sqrt(1 - v2/c2)

I don't get how they went from 2 to 3
t2 = c2t02/(c2-v2)

t2 = t02/(1-v2/c2)

Got it? (Divide top and bottom of the fraction by c2.)
 
  • #12
Oh oops thanks lol
 
  • #13
I got another problem, pls help: Inside a spaceship passing Earth at 0.6c, time goes slower inside the ship from the POV of earth. But, from the spaceship's POV the Earth is moving backwards at 0.6c so the Earth is the one whose time is slowing down?

The book claims this isn't a contradiction.. but how?
 
  • #14
I've said it before and I say it again: I don't like this example. I only get confused when I think of it. But there is a simpler example which demonstrates the relativity of simultaneity. I quote myself from another post:

"... imagine a light being turned on in the middle of the train. The light reaches the front and the back of the train simultaneously, according to an observer on the train. But according to an observer on the embankment, the light will reach the back of the train before it reaches the front of the train, because according to such an observer, the light that reaches the back of the train will have traveled a shorter distance than the light that reaches the front of the train, since train is moving, according to this observer."
 
  • #15
Nikitin said:
I got another problem, pls help: Inside a spaceship passing Earth at 0.6c, time goes slower inside the ship from the POV of earth. But, from the spaceship's POV the Earth is moving backwards at 0.6c so the Earth is the one whose time is slowing down?

The book claims this isn't a contradiction.. but how?
I think it is easier to see this if we think of a train instead of a spaceship. Again, I refer to another post of my own, where I try to explain this:

https://www.physicsforums.com/showthread.php?t=468826
 
  • #16
So if the Earth gets accelerated so much that it catches up to the spaceship and moves parallel to it at the speed 0.6c, Earthlings who launch themselves in rockets and visit the spaceship find out that the spaceship guys are old?

That.. can't be possible?
 
  • #17
Nikitin said:
So if the Earth gets accelerated so much that it catches up to the spaceship and moves parallel to it at the speed 0.6c, Earthlings who launch themselves in rockets and visit the spaceship find out that the spaceship guys are old?

That.. can't be possible?
As far as I undertand it, it will be as you write (provided that the rockets you mention have much smaller velocities than 0.6 c) because Earth is the body which accelerates in this case.

And well, I guess it wouldn't be possible to accelerate the Earth to the speed 0.6 c.:smile:
 
  • #18
Doc Al said:
Simultaneity is frame dependent.

But how can simultaneity be frame dependent when events themselves are frame independent? In other words, since events occur independently of any coordinates or frame, i.e., since events occur in only one way, simultaneity cannot be frame dependent.

I agree that light from events can reach observers in different frames differently, but what the heck has this got to do with the events themselves? I would say that it has everything to do with said observers physically separating during the observation, but nothing to do with how the events themselves actually occurred.

What say you?
 
  • #19
2clockdude said:
But how can simultaneity be frame dependent when events themselves are frame independent? In other words, since events occur independently of any coordinates or frame, i.e., since events occur in only one way, simultaneity cannot be frame dependent.
In SR. time is just a coordinate. The phenomenon is analogous to the following: If we rotate a cartesian coordinate system in the plane, two points which had the same x-coordinate before the rotation will have unequal x-coordinates after the rotation.
 
  • #20
2clockdude said:
But how can simultaneity be frame dependent when events themselves are frame independent? In other words, since events occur independently of any coordinates or frame, i.e., since events occur in only one way, simultaneity cannot be frame dependent.

I agree that light from events can reach observers in different frames differently, but what the heck has this got to do with the events themselves? I would say that it has everything to do with said observers physically separating during the observation, but nothing to do with how the events themselves actually occurred.

What say you?

Two events are separated by spacetime (otherwise there's only one event). How much time they are separated by is dependent on the observer's frame of reference.
 
  • #21
DaveC426913 said:
Two events are separated by spacetime (otherwise there's only one event). How much time they are separated by is dependent on the observer's frame of reference.

Your "time" is a coordinate value, but all physical phenomena are
completely independent of coordinates, because Nature quite clearly
doesn't need or use coordinates. Coordinates are merely tools of
description, and artifacts related to the choice of coordinates cannot
affect physical phenomena, only the _description_ of them.

Events can occur physically in only one way, regardless of how some
set of silly observers views the events by using light rays from them
or by using coordinates. Events can be either truly simultaneous or
not, and in Einstein's train example, he assumed that they were truly
or absolutely simultaneous. Why, then, did not both observers see
them as they really were? The only way that observers can actually
see how the events actually occurred is by placing truly synchronous
clocks _at_ the events. This is not done in relativity theory, is it?
 
  • #22
2clockdude said:
Events can be either truly simultaneous or
not, and in Einstein's train example, he assumed that they were truly
or absolutely simultaneous. Why, then, did not both observers see
them as they really were? The only way that observers can actually
see how the events actually occurred is by placing truly synchronous
clocks _at_ the events. This is not done in relativity theory, is it?
How do you define "truly simultaneous events" and "truly synchronous clocks"?

It seems that you believe that there exists an "absolute time" which is independent of all observers. It doesn't.
 
  • #23
The only "truly"* simultaneous events are events that occur coincident in both space and time.

(*is there another kind? falsely simultaneous?)

Now, how one distinguishes two events that are in the same spatial location at the same time is a tricky one. :wink:

2clockdude said:
Events can be either truly simultaneous or
not, and in Einstein's train example, he assumed that they were truly
or absolutely simultaneous.
No, he does not.

There is no such thing as absolute simultaneity in Einstein relativity.

In fact the relativity is short for 'relativity of simultaneity'. That is the central postulate of Einstein, from which all other phenomena are derived.
2clockdude said:
Why, then, did not both observers see
them as they really were? The only way that observers can actually
see how the events actually occurred is by placing truly synchronous
clocks _at_ the events. This is not done in relativity theory, is it?
It cannot be done.

There is no such thing as "really".

You are espousing Newtonian physics, which has been deprecated in favour of Einsteinian physics, as it better describes the universe we observe.
 
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  • #24
2clockdude said:
Your "time" is a coordinate value, but all physical phenomena are
completely independent of coordinates, because Nature quite clearly
doesn't need or use coordinates. Coordinates are merely tools of
description, and artifacts related to the choice of coordinates cannot
affect physical phenomena, only the _description_ of them.

Events can occur physically in only one way, regardless of how some
set of silly observers views the events by using light rays from them
or by using coordinates.
All true.
2clockdude said:
Events can be either truly simultaneous or not,
Not true, and you haven't given any argument why it should be.
2clockdude said:
and in Einstein's train example, he assumed that they were truly
or absolutely simultaneous.
Also not true.

In special relativity, two events can be related in one of three ways:
  1. if they have timelike separation, it is possible to travel from one to the other slower than the speed of light; an inertial observer will take the maximum time to travel, other observers will take a shorter time, but the time is never zero
  2. if they have null separation, it is possible to travel from one to the other in a straight line at exactly the speed of light;
  3. if they have spacelike separation, it is impossible to travel from one to the other; different inertial observers will disagree over whether they took place at the same time or not, or what order they occurred in
All observers (i.e. all coordinate systems) agree over which of the three types of separation applies to a given pair of events, whatever else they may disagree over.

Simultaneity is a coordinate-dependent property: it is simply the equality of two time coordinates. In general relativity, you are free to choose pretty much any coordinate system you like. The coordinates are just a set of 4 labels you apply to each event. In special relativity we deliberately restrict ourselves to using coordinate systems in which the speed of light is always the same value c. One we have adopted that constraint, we cannot also impose a constraint of simultaneity being absolute as those two constraints are not compatible with each over (as the train-lightning thought experiment shows).
 
  • #25
It's convenient to think of "simultaneity" as being an artifact of perception.

The short way to show this is to use the Einstein definition of simultaneity, which defines simultaneity in a specific frame as being defined by the midpoint method. You place a pair of stationary clocks at two different locations, and you synrhonize them via a signal emitted at the midpoint. The two events where the synchronizing signal reaches each clock are considered to be simultaneous.

That definition is all you need to show that simultaneity is relative in special relativity where the speed of light is always constant.

You can spend / waste a lot of time trying to come up with some "better" definition of simultaneity, the consequence of any "better" method would be to induce a perferred frame. But no experimental result has ever shown any reason to prefer one frame over another.

You could perhaps pick some particular frame by fiat and declare it to be "the one and true perferred frame", but if you actually try to calculate in it, you'll find it inconvenient to say the least.

For instance you could write down a Lagrangian using the generalized coordinates (I've done it, but I've never seen a published paper taking this approach). You'll find that the derived momenta in this formalism are not proportional to velocity, however, in the low velocity limit.

Basically, making Newtonian physics work in the low-velocity limit demands Einstein's clock synchronization procedure, which demands that the notion of simultaneity be frame-dependent.
 
  • #26
2clockdude said:
Coordinates are merely tools of
description, and artifacts related to the choice of coordinates cannot
affect physical phenomena, only the _description_ of them.
This is a key point. Since simultaneity means simply that [itex]t_a=t_b[/itex] you know immediately that simultaneity cannot affect physical phenomena, only the description.
 
  • #27
DaleSpam said:
This is a key point. Since simultaneity means simply that [itex]t_a=t_b[/itex] you know immediately that simultaneity cannot affect physical phenomena, only the description.

I would even go a little further. Strictly speaking, simultaneity does not describe (in a discrepant manner) the events, but the measurements that each observer carries out in order to solve the problems associated to those events. For example, "did the guys at the front at the back of the train get light signals emitted from the mid-point simultaneously?".

We say that, in the train frame, the signals were simultaneous. But what this describes, to be accurate, is that that those light signals have returned to the train-mid point simultaneously, the go-and-return trip has ben measured and hence it has been established that half of that time is the one that each of the front and back clock should read when they received their respective signals.

Similarly, we say that in the ground frame the said signals were not simultaneous. But actually, to be more precise, what we are describing here is that the signals did not return at the same time to the person who was standing in the ground by the train mid-point when they were emitted. That is why she did not set the ground clocks that were aligned by the train front and train back clock when they were illuminated, to read the same time.

That is semantics, yes, but helpful, I think. The descriptions are different but only because the described facts or events are different.

But what when it comes to describing the same events? Then both frames agree on the same words and descriptions. For example, how many times can the person at the back of the train scratch his nose in the time interval between receiving his or her signal and the one reflected from the front of the train? By applying the proper time formula, both frames reach the same conclusion and describe this event in a homogeneous manner.
 
  • #28
DrGreg said:
Originally Posted by 2clockdude
Events can be either truly simultaneous or not,

Not true, and you haven't given any argument why it should be.

The argument was given. It is the fact that events occur independently of frames and their clocks combined with the fact that relative simultaneity exists only when these clocks are used. The opposite of relative time is absolute time, so that exists when the other does not. But there is more to the simultaneity story; see below.

DrGreg said:
Originally Posted by 2clockdude

and in Einstein's train example, he assumed that they were truly or absolutely simultaneous.

Also not true.

You are wrong, and it's because you failed to read the whole train example story. I am not here to educate, but I will take the time to ask you what this phrase from that story means: "able meteorologist."

DrGreg said:
In special relativity we deliberately restrict ourselves to using coordinate systems in which the speed of light is always the same value c. One we have adopted that constraint, we cannot also impose a constraint of simultaneity being absolute as those two constraints are not compatible with each over (as the train-lightning thought experiment shows).

There is no evidence that light's one-way speed per two same-frame clocks is c in all frames. But there is evidence from Einstein himself that is not c in all frames when truly or absolutely synchronous clocks are used. Again, I am not here to educate, but look at Einstein's equation w = c - v at http://www.bartleby.com/173/7.html where he said that "The velocity of propagation of a ray of light relative to the carriage thus comes out smaller than c."

As promised above, here is the rest of the simultaneity story:
The only "proof" or "evidence" of the relativity of simultaneity is the train example.
However, it is easy to show that this example has nothing to do with the relative simultaneity of events.

Einstein believed that observers' different views of light rays from events say something about the events' occurrence times. It is easy to agree with Einstein when two events are involved because this makes it difficult to see what is really happening. However, if we look at only one event, e.g., the right-hand lightning strike, then we can clearly see Einstein's mistake.

Let's label the right-hand lightning strike event E. Let the rail observer be R, train observer be Tf, and an added rearward-moving train observer Tr.

-------------Tr--------R---------Tf-----------E
---------light<--------------------------------

The forward-moving train observer (Tf) sees the light ray before R, and Tr sees the ray after R. (These are absolute before-and-after's because these are three light-like events.) For example, Tf sees the ray at 11am, R sees it at noon, and Tr sees it at 1pm. (There are no clocks in the train example, but we can use these times to help us visualize the example. They merely echo the fact that the events have absolute before-and-after's.)

However, the observers now know that Einstein's view is false because a single event cannot occur at different times; that is, the observers must reject Einstein's belief that different views of a light ray from an event say something about the time of the event itself.

Why do the observers see the light ray arrive differently? The cause is simply the observers' physical separations. If the observers separate during the experiment, then the light ray must reach them differently, and this clearly has nothing to do with the time of the lightning event or simultaneity.

Here is Einstein's conclusion regarding his train example:
"Events which are simultaneous with reference to the embankment are not simultaneous with respect to the train, and vice versa (relativity of simultaneity). Every reference-body (co-ordinate system) has its own particular time; unless we are told the reference-body to which the statement of time refers, there is no meaning in a statement of the time of an event." http://www.bartleby.com/173/9.html

But we have found that seeing light rays from events differently says nothing about events' occurrence times or the RoS, but merely says that the observers were in different locations. The observers do disagree, but not about time or simultaneity, only about the light ray arrivals.
 
  • #29
2clockdude said:
The argument was given. It is the fact that events occur independently of frames and their clocks combined with the fact that relative simultaneity exists only when these clocks are used. The opposite of relative time is absolute time, so that exists when the other does not. But there is more to the simultaneity story; see below.



You are wrong, and it's because you failed to read the whole train example story. I am not here to educate, but I will take the time to ask you what this phrase from that story means: "able meteorologist."





There is no evidence that light's one-way speed per two same-frame clocks is c in all frames. But there is evidence from Einstein himself that is not c in all frames when truly or absolutely synchronous clocks are used. Again, I am not here to educate, but look at Einstein's equation w = c - v at http://www.bartleby.com/173/7.html where he said that "The velocity of propagation of a ray of light relative to the carriage thus comes out smaller than c."
How ironic that you accuse someone above of not having read the whole example, when you yourself obviously didn't read the whole section that you are quoting above. The quote comes from a part where he is discussing the state of physics before Relativity and is pointing out what,at the time, seemed a incompatibility between the propagation of light and the principle of Relativity. He then goes on later on the same page to state
"in reality there is not the least incompatibility between the principle of relativity and the law of propagation of light, " Put another way, he is giving a little background before going on to present his theory. He is not arguing for the statement you quoted. He hasn't even gotten to presenting his argument yet.
As promised above, here is the rest of the simultaneity story:
The only "proof" or "evidence" of the relativity of simultaneity is the train example.
However, it is easy to show that this example has nothing to do with the relative simultaneity of events.

Einstein believed that observers' different views of light rays from events say something about the events' occurrence times. It is easy to agree with Einstein when two events are involved because this makes it difficult to see what is really happening. However, if we look at only one event, e.g., the right-hand lightning strike, then we can clearly see Einstein's mistake.

Let's label the right-hand lightning strike event E. Let the rail observer be R, train observer be Tf, and an added rearward-moving train observer Tr.

-------------Tr--------R---------Tf-----------E
---------light<--------------------------------

The forward-moving train observer (Tf) sees the light ray before R, and Tr sees the ray after R. (These are absolute before-and-after's because these are three light-like events.) For example, Tf sees the ray at 11am, R sees it at noon, and Tr sees it at 1pm. (There are no clocks in the train example, but we can use these times to help us visualize the example. They merely echo the fact that the events have absolute before-and-after's.)

However, the observers now know that Einstein's view is false because a single event cannot occur at different times; that is, the observers must reject Einstein's belief that different views of a light ray from an event say something about the time of the event itself.

Why do the observers see the light ray arrive differently? The cause is simply the observers' physical separations. If the observers separate during the experiment, then the light ray must reach them differently, and this clearly has nothing to do with the time of the lightning event or simultaneity.

Here is Einstein's conclusion regarding his train example:
"Events which are simultaneous with reference to the embankment are not simultaneous with respect to the train, and vice versa (relativity of simultaneity). Every reference-body (co-ordinate system) has its own particular time; unless we are told the reference-body to which the statement of time refers, there is no meaning in a statement of the time of an event." http://www.bartleby.com/173/9.html

But we have found that seeing light rays from events differently says nothing about events' occurrence times or the RoS, but merely says that the observers were in different locations. The observers do disagree, but not about time or simultaneity, only about the light ray arrivals.

You are missing the whole point of the exercise. The railway observer sees the from both flashes simultaneously. and because he is halfway between the strike points, he can conclude that the strikes took place simultaneously.

He will also note that the train observer sees one flash before the other. (The train observer will be next to different points of the tracks when each flash reaches him).

Now, as you noted a single event can only occur once, so the train observer must also agree that he was next to two different points of the track upon seeing each flash and thus agrees that he sees the flashes at different times.

However, the train observer sits at the midpoint of the train, and the lightning strikes hit the end of the train. Due to the invariance of the speed of the light, the flashes approaching from each end of the train have to travel at the same speed relative to him as determined from his frame. If the light from the rear of the train approaches at 300,000 km/sec, and the light from the front of the the train approaches at 300,000 km/sec and the distances from from the observer to the two ends are equal, and he sees the flashes at different times, then he must conclude that the strikes occurred at different times.

The fact that the train observer see the flashes at the "same time" as the embankment observer is a red herring.

In fact, we can rearrange the experiment so that both observers do see the flashes at the same time. by changing the scenario so that the flashes arrive at the embankment observer at the same time as he is next to the train observer, like this:

[URL]http://home.earthlink.net/~jparvey/sitebuildercontent/sitebuilderpictures/train1.gif[/URL]

The expanding circles represent the flashes.

Again, according to the embankment observer, the flashes both occur simultaneously and he sees them simultaneously.

The train observer also sees them simultaneously. However, he is moving with respect the embankment. Thus he will be closer to one lightning strike than the other when the strikes occur.

Again, since the speed of light must be constant for him, the light from the strikes expand out as even circles from points that maintain a constant distance from himself. (while the points on the embankment where the strikes occurred move away from these centers. )

Thus this is what happens according to the train observer:

[URL]http://home.earthlink.net/~jparvey/sitebuildercontent/sitebuilderpictures/train2.gif[/URL]

In order for him to see both flashes at the same time and at the same time as the embankment observer, the strikes that caused them have to occur at different times.

Thus even though both observers see the flashes simultaneously, One concludes that they originated at the same time and the other that they originated at different times
 
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  • #30
2clockdude said:
The argument was given. It is the fact that events occur independently of frames and their clocks combined with the fact that relative simultaneity exists only when these clocks are used.
Your premise, "events occur independently of frames", does not imply your conclusion. So it cannot be considered as an argument for your conclusion.

2clockdude said:
However, the observers now know that Einstein's view is false because a single event cannot occur at different times
Sure it can, even non-relativistically. For instance, I regularly schedule events which occur at 11:00 am my time and 5:00 pm in my German colleague's time. There is nothing wrong with me assigning a time coordinate of 11:00 and someone else assigning a time coordinate of 5:00 to the same event. A single event can occur at different times in different frames. That is basic everyday non-relativistic physics.
 
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