Length Contraction rearrangement

[mananvpanchal]

Now, take two events happened at rest in S' frame at O and B' time. When we transform the two events, we get O and B in S frame. We can again easily say that OB' > OB. So, we have to say that time elapsed between two events in S' frame is more than S frame. So time is running faster in moving frame than rest frame.

Time on a spacetime diagram is like the time shown on a clock--the shorter the length on the diagram, the less time is on the clock. So when you say that OB' > OB, you're saying that a clock at rest in a frame accumulates more time than one moving in that frame, correct?

OB' > OB. OB' is time elapsed in S' frame between two events at rest in S' frame. OB is time elapsed in S frame between two events at rest in S' frame.
Suppose, OB=1 and OB'=1.25, so there is more time elapsed in S' frame rather than S frame.
Does this not seems that in S frame time running faster than S' frame between two events which is at rest in S' frame?

A clock that has accumulated 1 unit of time on it in the same time that another clock has accumulated 1.25 units of time is running slower.

Suppose, a light clock at rest in S' frame. S' observer measure 1 unit between two hit with mirrors. Where the clock is moving relative to S frame, so S observer sees diagonal path and he measure 1.25 unit between two hit with mirrors. We can say OB'=1 and OB=1.25. So OB' < OB. So we can say that S's clock running slowly with respect to S. But here we are getting OB' > OB. So we have to conclude that S's clock running faster with respect to S.

EDIT: Doc Al, I have edited quote, now it contains link to post

 

[mananvpanchal]

Time Dilation:

Thanks Chestermiller. But my requirement is this.

And I want to understand now time dilation using any process you explain me with diagram or transformation.

 

[Doc Al]

Suppose, a light clock at rest in S' frame. S' observer measure 1 unit between two hit with mirrors. Where the clock is moving relative to S frame, so S observer sees diagonal path and he measure 1.25 unit between two hit with mirrors. We can say OB'=1 and OB=1.25. So OB' < OB. So we can say that S's clock running slowly with respect to S.

This is correct. According to the the S frame, the light travels a greater distance and thus requires more time; so S concludes that a clock stationary in S' must run slower than his own clocks.

But here we are getting OB' > OB. So we have to conclude that S's clock running faster with respect to S.

What example are you talking about? (If you use the quotes properly, they will contain a link to the original text.)

 

[mananvpanchal]

Doc Al, I have edited quote, now it contains link

 

[Doc Al]

Doc Al, I have edited quote, now it contains link

Please point to the exact example you're talking about. I suspect your example has nothing to do with light clocks and that you're just misinterpreting the meaning of the lengths.

 

[Doc Al]

In S frame if we want time dilation we start transformation from S frame, but if we want length contraction we have to start transformation from S' frame. Why?

If you want to set up a pair of events that illustrate time dilation only (and nothing else), then you have to set up special circumstances. (Such as a clock at rest in a frame.) Similarly, if you want to illustrate length contraction only, you'll have to set up events that measure the ends of some moving object at the same time.

In general, you'll need to apply length contraction, time dilation, and the relativity of simultaneity all at once. That's what the Lorentz transformations do for you.

This is the thing I cannot accept it. Our transformation process should be clear. We cannot have double standard.

What double standard? The Lorentz transformations give a crystal clear and unambiguous procedure for transforming between frames. And it applies to any events, not just special circumstances.

 

[Chestermiller]

Thanks Chestermiller. But my requirement is this.

Darkhorror's reply, #59 as amended by my reply #60, provides a specific example that you were asking for. I don't know what else could provide a better example.

 

[Chestermiller]

Thanks Chestermiller. But my requirement is this.

I hope you are aware that, aside from the input data, your "mirror problem" is exactly the same as the problem posed and solved by Darkhorror in reply #59. Just change his 0.5c to 0.6c, his 10 seconds to your 1.25 units, and his 8.666 seconds to your 1.0 units. Your ability to recognize this is important to your understanding.

Chet

 

[darkhorror]

Now, take two events happened at rest in S' frame at O and B' time. When we transform the two events, we get O and B in S frame. We can again easily say that OB' > OB. So, we have to say that time elapsed between two events in S' frame is more than S frame. So time is running faster in moving frame than rest frame.

Why are you taking two events if they happened at the same place and time? Seems to me that you could just call it one event. Do you mean two different events that happen in the same place, but different times in frame of reference S'? What are OB' and OB even testing the time difference between? Is there another event? Plus why do you say OB' > OB prime while saying the event is at rest with respect to S', then say S' is the moving frame? Is this what you are trying to describe below?

Suppose, a light clock at rest in S' frame. S' observer measure 1 unit between two hit with mirrors. Where the clock is moving relative to S frame, so S observer sees diagonal path and he measure 1.25 unit between two hit with mirrors. We can say OB'=1 and OB=1.25. So OB' < OB. So we can say that S's clock running slowly with respect to S. But here we are getting OB' > OB. So we have to conclude that S's clock running faster with respect to S.

EDIT: Doc Al, I have edited quote, now it contains link to post

The problem you are having is you are just trying to use math, without understanding the situation or how to use the math correctly. You can't just chose to deal with time dilation, you also need to factor in length contraction, when events happen in specific frames of reference.

Like try and look at the situation you just gave here, and let's say you have two points, x and y, which are moving at .5c in S' FoR. These points are .5 light seconds apart in S' FoR. S' has the light clock which takes 1 second for light pulse to be sent and return as above. This light clock sends out a light pulse when x is at the same point as the light clock. Then since in S' FoR y is only .5ls behind x and moving at .5c the light pulse and y get to the light clock at the same time.

 

[mananvpanchal]

I need to write this from starting of the thread.

Please, look at below image. This displays Galilean transformation.

There are three stationary points A, O, B in the S frame. We can define the points in S frame as A(x_a, t_a), O(x_o, t_o), B(x_b, t_b). Now suppose a frame S' is moving relative to the S frame with V speed. Using Galilean transformation we can define the same points in S' frame as A&#039;(x&#039;_a, t&#039;_a)=A(x_a-vt_a, t_a), O&#039;(x&#039;_o, t&#039;_o)=O(x_o-vt_o, t_o) and B&#039;(x&#039;_b, t&#039;_b)=B(x_b - vt_b, t_b). The A', O' and B' points are not skewed with respect to S' frame in Galilean transformation.

Note the important point that A', O' and B' is the same point A, O and B respectively but defined by S' co-ordinate system.

Please, look at below image. This displays Lorentz transformation.

There are three stationary points A, O, B in the S frame. We can define the points in S frame as A(x_a, t_a), O(x_o, t_o), B(x_b, t_b). Now suppose a frame S' is moving relative to the S frame with V speed. (Taking c=1) Using Lorentz transformation we can define the same points in S' frame as A&#039;(x&#039;_a, t&#039;_a)=A(\gamma (x_a-vt_a), \gamma (t_a-vx_a)), O&#039;(x&#039;_o, t&#039;_o)=O(\gamma (x_o-vt_o), \gamma (t_o-vx_o)) and B&#039;(x&#039;_b, t&#039;_b)=B(\gamma (x_b-vt_b), \gamma (t_b-vx_b)).

Note the important point again that A', O' and B' is the same point A, O and B respectively but defined by S' co-ordinate system. But now the points is skewed with respect to S' frame.

The stationary points A, O and B is defined in S frame and the same points defined as A', O' and B' in S' frame moving relative to S frame.

Now, we can explain time dilation.
O and A is stationary points in S frame at same location but at different time. S measures OA time duration between these points. O and A is rest points in S frame, so OA is proper time in S frame. S' defines that points as O' and A'. Now we want to know how much time duration S' measures between those points. We can get parallel line to x axis and we get C point on t axis. Or we can get parallel line to x&#039; axis and we get the same A point on t axis. But, there is no meaning to get point A again. So if we want to find time dilation we have to get parallel line to x axis and get C point. We can see that OA < OC. So time elapsed in S' frame is more than time elapsed in S frame between same points which is at rest in S frame. So we can say that time running slowly in S' frame than S frame.

Now, we come to length contraction.
O and B is stationary points in S frame at same time but at different location. S measures OB length between these two points. O and B is rest points in S frame, so OB is proper length in S frame. S' defines that points as O' and B'. Now we want to know how much length S' measures between those points. We can get parallel line to t axis and we get D point on x axis. Or we can get parallel line to t&#039; axis and we get the same B point on x axis. But, there is no meaning to get point B again. And I am stuck here... I don't know how to get length contraction. I don't know what I have to call O'B' as. But I know that OB is proper length measured by S frame between rest points in the same fame. And I am surely know that O'B' is not proper length between rest points in S' frame. O'B' is length measured by S' between rest points of S frame.

We cannot start derivation of length contraction by guessing O'B' as proper length between rest points in S' frame. It is not really. The whole idea to derive length contraction starting from S' frame is strange.

And the whole problem of discussion starts from here.
O' and B' is assumed as rest points in S' frame. But O' and B' is not at same time in S'. So we have to evolve idea to pick different time component for the points which is assumed as at rest in S' frame.
After derivation we get contracted length as OB in S frame. And we have discovered that OB is contracted length in S because S measure length at same time.

Again I don't know what I should call O'B' as. But I am sure that OB is proper length measured by S frame between rest points of S frame. And I am sure again that O'B' is length measured by S' between rest points of S frame.

That is why the title of the thread is "Length Contraction rearrangement".

 

[mananvpanchal]

Hello All. Just consider once the above post. I expect a comment at least.

 

[Chestermiller]

If you continue to insist on using Minkowski diagrams to help gain an understanding of length contraction and time dilation, then you need to at least learn how to use them correctly. Until you do, you are not only wasting your own valuable time (which I'm sure you don't want to do), you're also wasting everyone else's. Two points about Minkowski diagrams:
1. The events A and A' are not separate points on the Minkowski diagram. They are the same event, and must coincide on the diagram. The same goes for events O and B.
2. Equal values of Δt and Δt' do not correspond to equal increments along the t and t' axes on the diagram. Equal values of Δx and Δx' do not correspond to equal increments along the x and x' axes on the diagram.
Most standard texts on SR provide a description of how to use Minkowski diagrams.

Chet

 

[mananvpanchal]

If you continue to insist on using Minkowski diagrams to help gain an understanding of length contraction and time dilation, then you need to at least learn how to use them correctly. Until you do, you are not only wasting your own valuable time (which I'm sure you don't want to do), you're also wasting everyone else's. Two points about Minkowski diagrams:
1. The events A and A' are not separate points on the Minkowski diagram. They are the same event, and must coincide on the diagram. The same goes for events O and B.
2. Equal values of Δt and Δt' do not correspond to equal increments along the t and t' axes on the diagram. Equal values of Δx and Δx' do not correspond to equal increments along the x and x' axes on the diagram.
Most standard texts on SR provide a description of how to use Minkowski diagrams.

Chet

Then please, help me here to understand Minkowski diagrams correctly or provide me the text. I want to learn Minkowski diagrams and time dilation and length contraction from Minkowski diagrams.

 

[Doc Al]

Then please, help me here to understand Minkowski diagrams correctly or provide me the text. I want to learn Minkowski diagrams and time dilation and length contraction from Minkowski diagrams.

What textbook are you using to teach yourself special relativity?

 

[darkhorror]

And the whole problem of discussion starts from here.
O' and B' is assumed as rest points in S' frame. But O' and B' is not at same time in S'. So we have to evolve idea to pick different time component for the points which is assumed as at rest in S' frame.
After derivation we get contracted length as OB in S frame. And we have discovered that OB is contracted length in S because S measure length at same time.

Again I don't know what I should call O'B' as. But I am sure that OB is proper length measured by S frame between rest points of S frame. And I am sure again that O'B' is length measured by S' between rest points of S frame.

That is why the title of the thread is "Length Contraction rearrangement".

You just want to know how to get the length starting from known length at rest in S, moving to calculate that length in S'?

if so you just use length * 1/\gamma

 

[Doc Al]

Now, we come to length contraction.
O and B is stationary points in S frame at same time but at different location. S measures OB length between these two points. O and B is rest points in S frame, so OB is proper length in S frame. S' defines that points as O' and B'. Now we want to know how much length S' measures between those points. We can get parallel line to t axis and we get D point on x axis. Or we can get parallel line to t&#039; axis and we get the same B point on x axis. But, there is no meaning to get point B again. And I am stuck here... I don't know how to get length contraction. I don't know what I have to call O'B' as. But I know that OB is proper length measured by S frame between rest points in the same fame. And I am surely know that O'B' is not proper length between rest points in S' frame. O'B' is length measured by S' between rest points of S frame.

We cannot start derivation of length contraction by guessing O'B' as proper length between rest points in S' frame. It is not really. The whole idea to derive length contraction starting from S' frame is strange.

And the whole problem of discussion starts from here.
O' and B' is assumed as rest points in S' frame. But O' and B' is not at same time in S'. So we have to evolve idea to pick different time component for the points which is assumed as at rest in S' frame.
After derivation we get contracted length as OB in S frame. And we have discovered that OB is contracted length in S because S measure length at same time.

Again I don't know what I should call O'B' as. But I am sure that OB is proper length measured by S frame between rest points of S frame. And I am sure again that O'B' is length measured by S' between rest points of S frame.

That is why the title of the thread is "Length Contraction rearrangement".

The easiest way to illustrate length contraction using your diagram is to let O'B' represent a fixed length in S' (imagine it being a stick). If you want to see how S would measure the length of that stick you must draw the worldlines of the stick endpoints. Those are shown in your diagram as the slanted lines parallel to the t' axis. Now for S to measure the length of the stick, he must measure the positions of the endpoints of that stick at the same time. To do that, draw the horizontal line t = 0 and see where it intersects those world lines: The length of the stick measured in S will equal what you have shown as OB in your diagram.

If you want, you can do it the other way around. Let OB be a stick at rest in S. Draw the worldlines of its endpoints, which will be vertical lines in your diagram. Then see where S' will measure the ends of the stick at any given time by slicing those worldlines with a line parallel to the x' axis.

One thing to be careful about, as pointed out by Chestermiller, is that the units are not the same in S and S'. Done carefully, and properly accounting for units, you will always find that the length of a stick at rest in S' will be measured as shorter in S, and similarly, the length of a stick at rest in S will be measured as shorter in S'. That's how length contraction works.

Of course, all of this is trivially done with the Lorentz transformations.

I know you want to be able to 'derive' length contraction from the Minkowski diagrams, but realize that length contraction is already built into the diagrams by how you set up your coordinate systems. (You are implicitly using the Lorentz transforms when you draw a Minkowski diagram.)

 

[Jorrie]

Then please, help me here to understand Minkowski diagrams correctly or provide me the text. I want to learn Minkowski diagrams and time dilation and length contraction from Minkowski diagrams.

I have used the attached Minkowski spacetime diagram to explain what you have asked, so maybe it will help (and not distract) you. What you see is the orthogonal axes of the reference frame (x,ct) and the oblique axes of the relatively moving frame (x',ct'), with coordinates x,ct =1,1 indicated by the larger green bullet and x',ct'=1,1 by the larger red bullet.

Now look at where the line ct'=1 intersects the ct-axis and where the line x'=1 intersects the x-axis (smaller red bullets). Both time dilation and length contraction are demonstrated. The same happens where the line ct=1 intersects the ct'-axis and where the line x=1 intersects the x'-axis (smaller green bullets), because the effects are reciprocal.

The relative velocity used in the diagram was 0.4c.

 

[mananvpanchal]

Thanks to all of you guys. This seems that I am interpreting Minkowsky diagrams incorrectly. As I start interpreting it truly, the length contraction is no longer confusing to me.

Thanks again.