Reimagining the Big Bang: Exploring the Relationship Between Relativity and Time

In summary: I mean the time as viewed by an observer in another inertial frame.There is no difference between your proper time and the time as observed by someone else.
  • #1
AlbertE
32
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Hi - I am new here. Here goes.
Has anyone ever considered the fact that our "rate of second elapse" is created by our speed through spacetime as provided to our planet/solar system/galaxy by the big bang?
Am I of the opinion that the time we inherit is gathered from the speed we at which we are moving.
All rotational motion is taken into consideration - such as our speed around the sun, our speed around the hub of the Milky Way and back to Earth our own rotation.
If we were to stop all of these movements - then am I correct in thinking that our seconds would elapse instantaneoulsy? (Given that STOP is as far away from the speed of light as is possible? And that seconds last longer at the speed of light.)
Thanks
 
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  • #2
AlbertE said:
Hi - I am new here. Here goes.
Has anyone ever considered the fact that our "rate of second elapse" is created by our speed through spacetime as provided to our planet/solar system/galaxy by the big bang?

What do you mean by the "rate of second elapse", and how do you measure it?

For that matter, what is the "speed through spacetime", and how do you measure it?

Are you any relation to the poster known as "trepeidation" who seems to have similar ill-defined ideas? (He didn't explain himself, apparently he just did a hit-and-run posting).
 
  • #3
pervect said:
For that matter, what is the "speed through spacetime", and how do you measure it?

Wouldn't this be

[tex]U^\mu U_\mu = \eta_{\mu\nu}\frac{dx^\mu}{d\tau}\frac{dx^\nu}{d\tau}[/tex]

which is basically equal to 1, or c in SI units?
 
  • #4
masudr said:
Wouldn't this be

[tex]U^\mu U_\mu = \eta_{\mu\nu}\frac{dx^\mu}{d\tau}\frac{dx^\nu}{d\tau}[/tex]

which is basically equal to 1, or c in SI units?

It's hard to say, unless we hear more from the O.P. (original poster). I'm still waiting to see if he's going to show up, or whether this is yet another "hit and run" posting.
 
  • #5
You can't determine your speed in relation to anything without having a non moving point of reference, but how do you find such a point anyway. For all I know everything is moving at C and C is just 2C. To us it's C of course I think that's what's important.
 
  • #6
"rate of second elapse"
As I understand it - a second elapses at a slower rate as we approach the speed of light. Its measured with atomic clocks.
Is this not true?
"Hit and run poster" - I guess youve had a prob? Dont worry - I own 300 + domains and run many many boards on the net (its my living) - I aint here to hit n run or cause a prob.
I was just pondering on the concept of time dilation - and was hoping for a chat about whether or not our own "rate of seconds" (keeping with seconds as a unit) elapse at our perceived rate due to the speed we are moving away from the point of origin - which as I understand things - would be the big bang.
To clarify - if we were further away from the point of origin now - we would logically be moving faster - and therefore would our seconds take "longer to elapse"?
Im thinking that you can determine speed by using the initial big bang point of singularity as a point of reference - something which nobody has considered so far as I am aware.
To me - c - that's just a nice effect in an expanding sphere of matter.
I would rather see that as we travel back towards the point of origin, that our "rate of second elsapse" would accelerate as we subtract x from our speed of outbound motion from the blast - where x would be our speed measure towards the point of the blast.
Hey - I don't have all the answers - there's no need for "malformed ideas" and such.
In summary - is it recognised that our seconds are what they are in terms of rate of elapse due to our speed through the cosmos?
If we were moving faster - would they take longer to elapse?
I think they would - but was hoping for other more mathematical minds to confer.
 
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  • #7
AlbertE said:
"rate of second elapse"
As I understand it - a second elapses at a slower rate as we approach the speed of light. Its measured with atomic clocks.
Is this not true?

No, it isn't. YOu have severely misunderstood time dilation.

Your time (proper time) never change. Your time, as view BY OTHERS in another inertial frame, is the one that "dilates". So if you view another frame moving, you will see that the time in that frame appears to move slower. But observers in THAT frame sees no difference. They observe their proper time being the same as it should.

So when "we approach the speed of light", we see no such time dilation of our proper time.

Zz.
 
  • #8
But in the twins paradox - doesn't the traveller come back less aged than the stationary twin?
And an atomic clock - after a long flight will show a different time to its stationary partner on the ground?

Therefore the time taken for a second to elapse for the traveller is longer than that for the none traveller surely I've read this correctly?

If - in flight - the ground based atomic clock were to be handed to a traveller after a few weeks of flying with his own clock, the traveller himself would read two different times?
 
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  • #9
AlbertE said:
But in the twins paradox - doesn't the traveller come back less aged than the stationary twin?
And an atomic clock - after a long flight will show a different time to its stationary partner on the ground?

There for the time taken for a second to elapse for the traveller is longer than that for the none traveller surely I've read this correctly?

But THAT involves MORE than just straightforward time dilation due to approaching the speed of light. It involves speeding up, slowing down, i.e. accelerated motion! This isn't what you stated in the beginning. And including such motion is MORE COMPLICATED, something I truly believe you have not understood.

I strongly suggest you go back and look at elementary description of Special Relativity. Look again the SIMPLEST situation of two moving inertial frame and understand what is meant by time dilation in that situation FIRST. If you do not understand this, you cannot build on more complicated situations, and certainly not something involving accelerated motion.

Zz.
 
  • #10
K - I am here to learn.

Ignore acceleration for the moment - I haven't mentioned that.

Am I correct at all when I say that a clock on an object moving close to the speed of light will measure time differently (will run slower) than a clock which is not moving at anywhere near the same speed.

?

Surely that's correct - and is the absolute simplest I can make it?
 
  • #11
Albert if your on a rocket that is moving(from your frame of reference)away/towards a space station with a relativisticy velocity any clock on the space station will seem to run slower compared to your clock when you observe them.

But people on the space station will observe YOUR clock to run slower when THEY observe you.

So both the space station and you will say "your clock runs slower than mine"

This is because you can either think of it as the rocket moving and the space station is holding its position. Or the rocket is standing still and the space station is moving. Both are equaliy valid.
 
  • #12
AlbertE said:
K - I am here to learn.

Ignore acceleration for the moment - I haven't mentioned that.

Am I correct at all when I say that a clock on an object moving close to the speed of light will measure time differently (will run slower) than a clock which is not moving at anywhere near the same speed.

?

Surely that's correct - and is the absolute simplest I can make it?

Let's go back to the simplest basics.

I am in inertial frame A. You are in inertial frame B. I see you moving with velocity v. You see me moving with velocity v, but in opposite direction. Are we OK so far?

My clock moves "normally". My proper time doesn't do anything "weird". In your frame, you see your clock moving normally. Your proper time also doesn't do anything weird. Are we OK so far here?

But when I look at YOUR clock, it is slower than mine. But since there's nothing special about my reference frame, there's nothing to say that my reference frame is absolute. You can also argue that in your frame, you seem my clock moving slower than yours.

NOW do you see what I'm getting at? When you say "clock or time slows down", you HAVE to indicate an observation from WHOSE perspective! You cannot just say "... a clock on an object moving close to the speed of light will measure time differently (will run slower) ... " without indicating explicitly the observing reference frame, because the observer that is moving with the clock sees NO slowing down.

Zz.
 
  • #13
Let's not call it a rocket since that implies acceleration. Let's instead just 2 space stations moving apart from each other. That way, it is a symmetric situation since they are both inertial (and therefore equally valid in the SR regime) observers.
 
  • #14
Ok - I am happy with what you are saying here with reference to the observers and the perceived "no slowing" of a traveller watching his own clock - thanks.

Can I put this question to you.

There are 3 people on Earth - p1, p2, p3.

p1 and p2 have clocks.

p3 is a "steward of the experiment".

Gaining instant and constant speed just below c - p1 goes into space for a period of time measured by p2 of 3 years.

On p1 arriving at Earth (he flew in a circular path (a rather large one at that)) - p1 and p2 hand their clocks over to p3 - the steward.

P3 looks at the clocks.

Are they reading different times according to what the steward sees at the instant the clocks are handed over?
 
  • #15
AlbertE said:
On p1 arriving at Earth (he flew in a circular path (a rather large one at that)) - p1 and p2 hand their clocks over to p3 - the steward.

Again, you have introduced an acceleration component. Something moving in a circular path, no matter how big, is in an accelerated frame. Do you really want to do this?

An observer in an accelerated frame is no longer the same as the one in an inertial frame. The symmetry between the two travellers no longer exists.

Zz.
 
  • #16
Reworded.

Ok - I am happy with what you are saying here with reference to the observers and the perceived "no slowing" of a traveller watching his own clock - thanks.

Can I put this question to you.

There are 3 people on Earth - p1, p2, p3.

p1 and p2 have clocks.

p3 is a "steward of the experiment".

Gaining instant and constant speed just below c - p1 goes into space for a period of time measured by p2 of 3 years.

On p1 arriving at Earth (he flew straight out - and straight back) - p1 and p2 hand their clocks over to p3 - the steward.

P3 looks at the clocks.

Are they reading different times according to what the steward sees at the instant the clocks are handed over?
 
  • #17
First welcome to these Forums Albert!

In your last example p2 and p3 are the same are they not? It's just that p3 hasn't a clock.

p1 and p2 clocks will read differently, p1 will record less time duration. In that sense time dilation is 'real', it makes a physical difference.

The twin paradox depends on the fact that, as velocities are relative, p1 might think it was p2 and p3 who went on the journey with the whole Earth, and therefore p2's clock ought to read 'slow', whereas p2/p3 will think it was p1 who made the trip and her clock ought to be 'slow'.

However, the paradox is resolved by realising that, although velocities are relative, accelerations are not; you can tell whether it was p1 or p2/3 who took a trip, p1 accelerated outwards and then accelerated 'inwards' to get back home again. It is p1's clock that is slow compared to the other two.

If you want a real 'twin' paradox consider two space travellers who circumnavigate a closed universe. They pass close by each other at high relative speed and synchronise their clocks. Neither accelerate or decelerate, they both remain in inertial frames of reference. After a very long time they pass by each other again, one having circumnavigated the universe, and compare clocks a second time. Which one made the circumnavigation? From the point of view of each both would consider that they had remained stationary and the other accomplished the circumavigation, each would think the other's clock would be 'slow', but which one?

Garth
 
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  • #18
AlbertE said:
On p1 arriving at Earth (he flew straight out - and straight back) - p1 and p2 hand their clocks over to p3 - the steward.

Again, this requires a slowing down, and then an acceleration in the opposite direction, i.e. ACCELERATION/DECELERATION.

This is no different than your earlier example which I said contained accelerating frame. You already said you don't want this, so why are you invoking it again?

Zz.
 
  • #19
ZapperZ
It assumes instant speed and instant stop and instant change of direction - this is more than sufficient in order to answer the question.

Would the answer be different if we involved acceleration/deceleration - possibly under certain rates of those - and time traveling close to c.

Thank you Garth - I'll post again once I get my head around a few matters.
 
  • #20
AlbertE said:
ZapperZ
It assumes instant speed and instant stop and instant change of direction - this is more than sufficient in order to answer the question.
A change of velocity is an acceleration, even if it is "instant". Instant change of velocity just implies infinite acceleration.
 
  • #22
AlbertE said:
ZapperZ
It assumes instant speed and instant stop and instant change of direction - this is more than sufficient in order to answer the question.

If you are assuming that, then why not go all the way and make other outrageous assumption, such as going beyond c? Why stop there?

This is not a reasonable assumption. You cannot apply bits and pieces of physics and discard the rest.

Zz.
 
  • #23
I didnt try and convince - I merely asked a question.

Zapper - you didnt answer -

"Would the answer be different if we involved acceleration/deceleration - possibly under certain rates of those - and time traveling close to c."

Please remember, I don't need to know "how" different the clocks are - simply if they are different or not.
 
  • #24
"Dear AlbertE (I hope you are not really identifying yourself with this great man)"
Am I Heckers! :)
Its just a sign on.
 
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  • #25
"A change of velocity is an acceleration, even if it is "instant". Instant change of velocity just implies infinite acceleration."

I know :)

I just thought I'd keep it simple in my mind until I was 100% certain the clocks would read differently - as read by person 3 - the "steward".

Im not a Nobel Prize winner - I am just poking round about space and time really (obvious).

I'd like to learn a few things - not teach! :)

Getting a bit fed up with the Discovery Channel and Astonomy books.
 
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  • #26
Albert read the link Mortimer posted it clears that question up very good
 
  • #27
Its ok Azael - I have had the answer - nothing too deep at all by your standards on here - but the answer that :-

The clock which travels will read behind the clock which did not.

Is absolutely fine for me for the mo.

:)
 
  • #28
AlbertE said:
I didnt try and convince - I merely asked a question.
Zapper - you didnt answer -
"Would the answer be different if we involved acceleration/deceleration - possibly under certain rates of those - and time traveling close to c."
Please remember, I don't need to know "how" different the clocks are - simply if they are different or not.

See, this is what I find very annoying. You are changing the "rules" as you go along. First you are doing purely inertial frame. But you are using an example with an accelerated frame. When I told you that, you said no, let's not do accelerated frame. But you continue to use examples that had accelerated frames. And now, after being confronted by the fact that your "thought experiments" are NOT inertial, but rather accelerated frames, you now want to do that.

I think you have no clue what you want. When faced with that, how is one supposed to answer a question that you can't form? I can't give you an answer because I do not know the EXACT parameter that is involved in the situation, because you yourself are not clear what exact are involved.

An undefined question deserves an ambiguous answer. I think you just received one.

Zz.
 
  • #29
I think you will find that the answer I have been given is quite accurate - and bypasses any misgivings in my question.

However - please feel free to enlighten me if the answer I have been given is wrong.
 
  • #30
There is more to a question than just the answere. A answere alone doesn't give any real knoweledge. To really understand you must know how to get the answere and that as far as I can tell(havent been a member for so long)is the purpose of this forum. Thats why some get a bit ticked off with questions where people only want the answere not the knoweledge.

Hope you decide to dig deeper. Its well worth it :)
 
  • #31
AlbertE said:
"rate of second elapse"
As I understand it - a second elapses at a slower rate as we approach the speed of light. Its measured with atomic clocks.
Is this not true?

I see we've had a lot of responses in the meantime...

This remark is close to being true, but you actually need two clocks to determine what you are calling the "rate of second elapse".

It may be a bit obvious, but when you compare a clock to itself, it always ticks at 1 second per second.

To come up with a number different than 1, you must compare your clock to someone else's clock.

But the first question you have to ask is "which clocks are being compared?" And the next question involves "how do we compare them".

For cases involving gravitational time dilation, there are easy answers to both of these questions. We compare our clock in a gravity well to a distant clock outside the gravity well, and the round-trip time is a constant, so there is no real issue on how to compare the rate of the clocks.

Things are not nearly so easy for two clocks, sitting in space, both moving.

One of the basic principles of relativity is that it is impossible to tell who is moving, and who is standing still.

One highly non-intuitive consequence of this is that from the point of view of twin A and twin B, who are moving relative to each other, is that A thinks B's clocks are runnign slow, and B thinks A's clocks are runnign slow. And they are both, in some sense, correct.

This is known as the "twin paradox". There has been a lot written about its resolution, the key point turns out to be that there isn't actually a standard way to compare the rate of separated clocks that are moving relative to each other. "Which clock is slow" depends on the mechanism of the comparison operation.

For instance, suppose you compare clocks by bringing them physically back to the same point in space. Then one of the clocks, A or B, must accelerate.

If A and only A accelerates, it will have the least elapsed time. If B and only B acclerates, it will havea hte least elapsed time.
 
  • #32
AlbertE said:
Im thinking that you can determine speed by using the initial big bang point of singularity as a point of reference - something which nobody has considered so far as I am aware.
To me - c - that's just a nice effect in an expanding sphere of matter.
I would rather see that as we travel back towards the point of origin, that our "rate of second elsapse" would accelerate as we subtract x from our speed of outbound motion from the blast - where x would be our speed measure towards the point of the blast.

You are on the initial big bang point. That is the meaning of the big bang theory. All the points in space were at the moment of the big bang the central point. There is no special point in the universe. I find very good the analogy of the expanding balloon were the space is the surface of the balloon and the original point is in the centre of the balloon, i.e. a point in space-time outside the current spatial hyper surface and not on it and the place that all the points of the balloon occupied at the initial moment.
 

What is the Big Bang theory?

The Big Bang theory is a scientific explanation for the origin and evolution of the universe. It suggests that the universe began as a singularity, a point of infinite density and temperature, and has been expanding and cooling ever since.

How does relativity relate to the Big Bang theory?

Einstein's theory of relativity plays a crucial role in understanding the Big Bang. It explains how space and time are interconnected and how the fabric of space-time can be warped by massive objects, such as black holes. This is important in understanding the expansion of the universe and the concept of cosmic inflation.

What is the relationship between time and the Big Bang?

The Big Bang theory suggests that time began with the universe, so there is no "before" the Big Bang. However, as the universe expands and cools, time also changes. This is known as the arrow of time, and it is thought to be linked to the increase in entropy, or disorder, in the universe.

How has our understanding of the Big Bang changed over time?

Our understanding of the Big Bang has evolved over time as new evidence and theories have emerged. Initially, the Big Bang was thought to be a sudden explosion, but now it is believed to have been a rapid expansion. Additionally, the concept of cosmic inflation has been incorporated into the theory, which helps explain certain observations, such as the uniformity of the cosmic microwave background radiation.

What are some current areas of research in the study of the Big Bang?

Scientists are currently exploring various aspects of the Big Bang, such as the nature of dark matter and dark energy, the possibility of multiple universes, and the role of quantum mechanics in the early universe. Additionally, there is ongoing research into the cosmic microwave background radiation and the formation and evolution of galaxies and large-scale structures in the universe.

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