Trouble with Lorentz transformations

In summary, the conversation discusses using Lorentz transformations to derive the "length contraction" result. It is noted that the incorrect result is obtained because the measurements are not simultaneous in the unprimed frame. The correct result is then derived using the equations x' = γ(x - vt) and t' = γ(t - vx/c²). This leads to the conclusion that L' = γL, where L' is the length measured by the primed frame and L is the length measured by the non-primed frame.
  • #36
stevmg said:
x2 = 1.25(12 + 0.6*0) = 15 ly
t2 = 1.25(0 + 0.6*12) = 9 yr

Those calculations are correct. So now you know that in the unprimed frame, the left end of the rod is at [itex]x_1 = 0[/itex] at [itex]t_1 = 0[/itex], and the right end of the rod is at [itex]x_2 = 15[/itex] at [itex]t_2 = 9[/itex]. You want to find the length of the rod in the unprimed frame, but you can't simply take the difference [itex]x_2 - x_1 = 15 - 0 = 15[/itex], because [itex]x_1[/itex] and [itex]x_2[/itex] are "measured" at different times, and the rod has moved in between. So you need to "correct" the position of one end of the rod to make the times match.

In the unprimed frame, the left end of the rod is at [itex]x_1 = 0[/itex] at [itex]t_1 = 0[/itex], and is moving to the right with speed 0.6. Where will it be (what is [itex]x_1[/itex]) nine yr later (at [itex]t_1 = 9[/itex]), and what is [itex]x_2 - x_1[/itex] at [itex]t_1 = t_2 = 9[/itex]?

Or instead, you can "correct" the position of the right end of the rod. At [itex]t_2 = 9[/itex], it's at [itex]x_2 = 15[/itex] and is moving to the right with speed 0.6. Where was it nine yr earlier (at [itex]t_2 = 0[/itex]), and what is [itex]x_2 - x_1[/itex] at [itex]t_1 = t_2 = 0[/itex]?
 
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  • #37
stevmg said:
itbell and/or starthaus -

Moving right along:

We will need [tex]\gamma[/tex] for furture calculations.

[tex]\gamma[/tex] = 1/[tex]\sqrt{1 - v^2/c^2}[/tex] = 1/[tex]\sqrt{1 - 0.6c^2/c^2}[/tex] = 1/[tex]\sqrt{1 - 0.36}[/tex] = 1/[tex]\sqrt{0.64}[/tex] = 1/0.8 = 1.25

From Lorentz,
x1 = [tex]\gamma[/tex](x1' + vt1')
x2 = [tex]\gamma[/tex](x2' + vt2')

t1 = [tex]\gamma[/tex](t1' + vx1'/c2)
t2 = [tex]\gamma[/tex](t2' + vx2'/c2)

x1' = 0, t1' = 0
x2' = 12, t2' = 0
x1 = 0, t1 = 0

v = 0.6, [tex]\gamma[/tex] = 1.25

Now to calculate x2 and t2:

x2 = 1.25(12 + 0.6*0) = 15 ly
t2 = 1.25(0 + 0.6*12) = 9 yr

The correct formula is:
x2 = (x'2 + vt'2) - from above post by starthaus
to starthaus - isn't that what I wrote in this part (see the last line in the above quote?)
If so, then 15 ly is a correct calculation and so would be the 9 years for t2 = 1.25(0 + 0.6*12) = 9 yr. However, I would have to adjust backwards the length at t = 0 (in other words -9*0.6 = -5.4. 15 - 5.4 = 9.6, so the length x2 when t = 0 was actually 9.6 ly.

Guess what, uising the length contraction formula we get the same result. 12 * (1/[tex]\gamma[/tex]) = 12/1.25 = 9.6 ly.

stevmg said:
Now, something is wrong.

If I use 9 as t2 and v = 0.6, x2 = 0.6*9 = 5.4 ly. That makes more sense. What is wrong with the equation for x2?

I am missing something...

Just tell me, at least, does t2 = 9? Does x2 = 5.4 ly?


Yes, starthaus, I know this is wrong and I think my calulations above go along with you but please give a thumbs up or another correction, if necessary.

stevmg said:
Ooooooh, I just got it. According to starthaus I want to set t1 = t2 = 0. When you do that, (x2' - x1') = [tex]\gamma[/tex](x2 - x1)
or 12 ly = 1.25 (x2 - x1)
(x2 - x1) = 9.6 ly. If x1 = 0, then x2 = 9.6
If x1' = 0, x2' = 12
t1' = 1.25(0 - 0.6*0) = 0
t2' = 1.25(0 - 0.6*9.6) = -7.2 yr

Now, does that make any damn sense? Please explain to me how that would happen?

I assume my calculations must be wrong - somewhere.

Actually, using t1 = t2 = 0 as per starthaus gives these weird answers, but the "proper time" both ways comes out the same:

SQRT[(-7.2 - 0)2 - (12 - 0)2] = [tex]\sqrt{-92.16[/tex]

and

SQRT[(0 - 0)2 - (9.6 - 0)2 = [tex]\sqrt{-92.16[/tex]
 
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  • #38
stevmg said:
Actually, using t1 = t2 = 0 as per starthaus gives these weird answers, but the "proper time" both ways comes out the same:

[tex]\sqrt{(-7.2 - 0)^2 - (12 - 0)^2}[/tex] = [tex]\sqrt{-92.16[/tex]

and

[tex]\sqrt{(0 - 0)^2 - (9.6 - 0)^2}[/tex] = [tex]\sqrt{-92.16[/tex]

it is getting worse and worse. Somehow you manage to twist and missapply everything I tried to teach you. One more time, you can EITHER:

1. Calculate [tex]x_1-x_2[/tex] for [tex]t_1=t_2[/tex]

OR

2. Calculate [tex]x'_1-x'_2[/tex] for [tex]t'_1=t'_2[/tex]

In EITHER case you must apply ONLY the Lorentz transforms. IF you do the things right, you will get:

1. [tex]x_1-x_2=(x'_1-x'_2)/\gamma[/tex]

OR

2. [tex]x'_1-x'_2=(x_1-x_2)/\gamma[/tex]

It is that simple.
 
  • #39
starthaus said:
you can EITHER:

1. Calculate [tex]x_1-x_2[/tex] for [tex]t_1=t_2[/tex]

OR

2. Calculate [tex]x'_1-x'_2[/tex] for [tex]t'_1=t'_2[/tex]

In EITHER case you must apply ONLY the Lorentz transforms. IF you do the things right, you will get:

1. [tex]x_1-x_2=(x'_1-x'_2)/\gamma[/tex]

OR

2. [tex]x'_1-x'_2=(x_1-x_2)/\gamma[/tex]

It is that simple.

Starthaus - I will go back to post 1 of pc2-brazil and go through your steps again but using my numbers.

I knew that when I was getting square roots of negative numbers for "proper times", albeit that they were "equal" I knew I was in the spacelike area of the spacetime coordinate system. I guess I "proved" that one cannot be in two places at the same time no matter how fast you travel but two different points (the beginning and end of a rod) can be in two different places at the same time, which is the direction you are trying to send me.

Now, did you see my post about "Clocks and Rods in Motion" above from Einstein's Relativity, Section XII?

Any thought on that equation:

t = x/[tex]\sqrt{1 - v^2/c^2}[/tex]

Is that right? Dr. Einstein did not go through the algebraic derivation of that equation based on his preceding paragraphs. Should it be t = t'/[tex]\sqrt{1 - v^2/c^2}[/tex]?
 
  • #40
A simple check of dimensions will give you the answer. Gamma is a dimensionless quantity so on the left we have the dimensions of time and on the right side dimensions of length. This is impossible. Whenever in doubt, check the dimensions if they are not the same on both sides it is wrong.
 
  • #41
Cyosis -

It would appear that my edition of Relativity has a misprint as this has the form of
t = [tex]\gamma[/tex]x.

Mine is the Tess edition (15th edition) of Relativity, The Special And General Theory
ISBN: 1-57912-515-8. I will have to go to the library and look up a totally different edition of the same works and see if this "misprint" exists there, too.

Steve G
Melbourne, FL
 
  • #42
stevmg said:
Now, did you see my post about "Clocks and Rods in Motion" above from Einstein's Relativity, Section XII?

Any thought on that equation:

t = x/[tex]\sqrt{1 - v^2/c^2}[/tex]

Is that right? Dr. Einstein did not go through the algebraic derivation of that equation based on his preceding paragraphs. Should it be t = t'/[tex]\sqrt{1 - v^2/c^2}[/tex]?

yes, it is a typo
 
  • #43
To starthaus:

Using the algebraic derivation below by pc2-brasil, the answer becomes thus:

[tex]x_2' = 12, x_1' = 0[/tex], v = 0.6c
[tex]x_2 - x_1 = \(1/\gamma)*(x_2' - x_1')[/tex]
[tex]\gamma[/tex] = 1/[tex]\sqrt{1 - v^2/c^2}[/tex] = 1/[tex]\sqrt{1 - v^2/c^2}[/tex]
= 1/[tex]\sqrt{1 - (0.6c)^2/c^2}[/tex] = 1.25
[tex](x_2 - x_1) = (x_2' - x_1')/\gamma[/tex] = (12 - 0)/1.25 = 9.6 ly


pc2-brazil said:
Thank you, I understand it now.
So, in order to derive the length contraction result using the transformation with t' (x = γ(x' + vt')), I have to find the relation between t'1 and t'2, knowing that t1 = t2:
[tex]t_1=\gamma(t'_1+vx'_1/c^2)[/tex]
[tex]t_2=\gamma(t'_2+vx'_2/c^2)[/tex]
[tex]t_1=t_2[/tex]
[tex]\gamma(t'_1+vx'_1/c^2)=\gamma(t'_2+vx'_2/c^2)[/tex]
[tex]t'_1+vx'_1/c^2=t'_2+vx'_2/c^2[/tex]
[tex]t'_2-t'_1=-\frac{v(x'_2-x'_1)}{c^2}[/tex]
Now, I can make x2 - x1:
[tex]x_2-x_1=\gamma(x'_2+vt'_2-x'_1-vt'_1)[/tex]
[tex]x_2-x_1=\gamma[x'_2-x'_1+v(t'_2-t'_1)][/tex]
Substituting the expression found for (t'2-t'1)
[tex]x_2-x_1=\gamma\left[x'_2-x'_1-\frac{v^2(x'_2-x'_1)}{c^2}\right][/tex]
[tex]x_2-x_1=(x'_2-x'_1)\gamma(1-\frac{v^2}{c^2})[/tex]
[tex]x_2-x_1=(x'_2-x'_1)\gamma\times\gamma^{-2}[/tex]
[tex]x_2-x_1=\frac{x'_2-x'_1}{\gamma}[/tex]
which is the length contraction result.
This same result can be obtained in a faster way by using x'1 = γ(x1 - vt1) and x'2 = γ(x2 - vt2), and calculating x'2 - x'1 with t1 = t2.

I can do it in steps and I did just that in my post (#37) and got the right answer (9.6 ly) but the intermediate steps looked weird but were mathematically correct. You thought I was screwing up but I wasn't. I was going up the hill a different way but I still got to the top. If you don't believe me, query itbell as he or she told me to do it this way.

Also, my "proper time" calculations based on the "weird" results where we reached the same square root ([tex]\sqrt{-92.16}[/tex] also confirms the calculations. x2 - x1 = 9.6 ly
and that is exactly what your method did but not the same way.

Your method is a lot easier and pc2-brazil's algebra derives the general approach to this problem.

pc2-brazil thanked you in advance. I have to thank you after-the-fact.

By the way, my user name (stevmg) isn't too secret coded. I've been around a long time.

Steve G
Melbourne, FL
 
  • #44
Cyosis:

It's a misprint.

I found the same book online in .pdf format and the equation
t = [tex]\gamma[/tex]x should be t = [tex]\gamma[/tex]*1 or

t = 1/[tex]\sqrt{1 - v^2/c^2}[/tex]

He's actually comparing what t is for t' = 0 and t' = 1

Makes sense as one second in "moving" time is greater than 1 second in "stationary" time.

I know, there is NO preferred frame of reference, but this compares one that is moving (O') with one that is "stationary" (O)
 
  • #45
I know it is a misprint I told you in post 40 and gave you a simple procedure for checking such things. If t is a time that new equation doesn't make any sense dimensionally either unless 1 has the unit of time somehow.
 
  • #46
Actually, Cyosis, you told me how to check for the error. In other words you implied it was in error but didn't say it was. Now I couldn't conceive of Dr. Einstein publishing a book with such an error. So, I wanted somebody else out there who actually saw it printed correctly to tell me so as I had only one book at my disposal. The .pdf "book" on line confirmed that it was a typo.

When I was in charge of teaching residents in Pediatrics, one of my staff had the habit of telling the residents "You might want to do something (whatever the something was." What he meant was "Do this something." Not "You might want to..." I had to correct him many times and tell him, "iIf you want to tell someone to do something, don't suggest it, tell them." That's where I am coming from. You have to tell me something in an idiot-proof fashion or I will find the idiot's way to screw it up. Years of experience in this regard.

Thanks for all your help so far and that goes to
starthaus
itbell
Fredrik
DaleSpam
JesseM
and all the others
 
  • #47
Perhaps I didn't spell it out. The main point of my post was to provide you with a method you can use to check an equation. I can't stress enough how helpful dimensional analysis is. It won't prove that an equation is correct, but if the dimensions on the left don't equal the dimensions on the right you know for sure the equation is wrong. Anyhow I don't want to go off topic too much, but it's important to learn to review your or someone else's results and ask yourself if they make sense.
 
  • #48
Hey, Cyosis -

No problem. I get it. When I took Physics and Chemistry in high school and college, that was one way we would keep tabs on any gross errors in equations.

BUT...

When it came to me to even question Dr. Einstein (or a book he authored) I was a little hesitant to assume anything and sought to get additional information. As it turns out, my questioning was justified and starthaus and you confirmed this. Good to see, though, that it was a misprint and not Dr. Einstein.

What I said about the residents was true - I always gave them "no s--t" instructions whenever I wanted them to do something. I never implied anything. In medicine, if something can be done wrong, it will be.

Makes you really confident of health care, right?
 
  • #49
stevmg said:
What I said about the residents was true - I always gave them "no s--t" instructions whenever I wanted them to do something. I never implied anything. In medicine, if something can be done wrong, it will be.

Always safest to be explicit. Ask the blacksmith who took a red hot horse shoe from the fire and said to his apprentice, "When I nod my head, hit it hard with the hammer."
 
  • #50
Oh my God!

Langauge is not precise. No way it can be made to be. Sometimes over explicitness can be too cumbersome but common sense still prevails.

Sometimes there just is no cure for stupid and I "ain't" so smart.

Langauge Myths by Laurie Bauer & Peter Trudgill.
 
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  • #51
stevmg said:


The correct formula is:
x2 = (x'2 + vt'2) - from above post by starthaus
to starthaus - isn't that what I wrote in this part (see the last line in the above quote?)
If so, then 15 ly is a correct calculation and so would be the 9 years for t2 = 1.25(0 + 0.6*12) = 9 yr. However, I would have to adjust backwards the length at t = 0 (in other words -9*0.6 = -5.4. 15 - 5.4 = 9.6, so the length x2 when t = 0 was actually 9.6 ly.

Guess what, uising the length contraction formula we get the same result. 12 * (1/[tex]\gamma[/tex]) = 12/1.25 = 9.6 ly.

I can't follow all your numerical calculations, as a rule, you should be able to express your ideas in symbolic form. I repeat, you have no right to write what amounts to [tex]x_2=v*t[/tex] since [tex]v [/tex] is the speed between the frames.

Actually, using t1 = t2 = 0 as per starthaus gives these weird answers, but the "proper time" both ways comes out the same:

SQRT[(-7.2 - 0)2 - (12 - 0)2] = [tex]\sqrt{-92.16[/tex]

and

SQRT[(0 - 0)2 - (9.6 - 0)2 = [tex]\sqrt{-92.16[/tex]

I never wrote such stuff, nor did I direct you to. Negative proper time is a clear indication of another error in your calculations.
 
  • #52
Let's put this to bed:

To wit, assume that there are two reference frames O (the "stationary" one) and O' (the "moving" one.) The moving frame (O') is going at 0.6c to the right.
The length of the rod is (in this example) 12 ly in the O' frame and is stationary with respect to the O' frame. This is a specific case of the x2' - x1' which pc2-brazil discusses. v = 0.6c and is the speed between the frames with O stationary and O' moving at the 0.6c to the right.
Thus, gamma is 1.25.
[tex]\gamma[/tex] = 1/[tex]\sqrt{1 - v^2/c^2}[/tex]
[tex]\gamma[/tex] = 1/[tex]\sqrt{1 - (0.6c)^2/c^2}[/tex]
[tex]\gamma[/tex] = 1/[tex]\sqrt{1 - 0.36[/tex]
[tex]\gamma[/tex] = 1/[tex]\sqrt{0.64[/tex] = 1/0.8 = 1.25
By convention, we will assume that all measurements and times start from x = 0, x' = 0, t = 0 and t' will calculate to zero which we will see below.
By the specific example I gave, we were given a specific length in O' which I chose to be 12 ly. This would represent x2' - x1' as stated a few paragraphs above.
x1 = 0, t1 = 0
x1' = [tex]\gamma[/tex]*(x1 - v*t1) = 1.25(0 - 0.6*0) = 0 If I am not mistaken then this is the correct Lorentz transformation regarding distance.
t1' = 1.25(t1 - v*x1) = 1.25(0 - 0.6*0) = 0 Likewise, this should be the correct Lorentz transformation with regards to time.
By the conditions imposed in the discourse between starthaus and pc2-brazil, t1 = t2. This was so because the L = (x2 - x1) was being measured or calculated in the stationary frame given the measure of L' = (x2' - x1') which is the length in the moving frame (or O').
t1 = t2 = 0. This is my adaptation of the requirement that t1 = t2.
Because of the relativity of simultaneity one cannot assume that t1' = 0, so this must be calculated, if you need it. The question did not ask for t2' but merely for the value of x2 - x1. We will use the given that t1 = t2 and with that we are to calculate x2 - x1. This means (and pc2-brazil states so) we are given x2' - x1' and which, in my particular case here, is 12 ly as stated above. Because of the values of x1 = 0, t1 = 0 and, x1 = 0 and t1' = 0 which are stated above, all we need to find is x2 which will then be the value of x2 - x1. We can calculate t2' which will give the value of t2' - t1'. Again, this was not asked for but doing this reveals some interesting intermediate results which only makes sense in the time-space Minkowski system.

We develop two equations in two unknowns which will give us answers for x2
(which is the answer we are after) and t2' which we can accompish at the same time.

Equation 1:
x2 = [tex]\gamma[/tex]*[(x2' - x1') + vt2'] Now, I am positive that this is the correct form of the Lorentz transformation when going from O' back to O.
x2 = 1.25*[12 ly + (0.6)t2']
Equation 2:
t2' = [tex]\gamma[/tex]*[t2 -vx2] = 1.25*[0 - (0.6)x2]
t2' = -1.25*0.6x2
t2' = -0.75x2
substituting equation 2 into equation 1:
x2 = 1.25[12 ly + (0.6)(-0.75x2]
1.5625x2 = 15 ly
We divide both sides by 1.5625 and we get:
x2 = 9.6 ly
This also represent (x2 - x1) = L from pc2-brazil. This is because x1 = 0, so the value of x2 is the L.
This is the right answer and does equal L'/[tex]\gamma[/tex] or 12/1.25 which is the original pc2-brazil notation.

If we back substitute x2 = 9.6 ly into t2' = -0.75x2 we get t2' = -7.2 yr.

I also derived using the above equations but substituting for x2 with t2' into equation 1 and proceeded to solve the new equation for t2'. This likewise came out with the same answer: -7.2 yr.

pc2-brazil's algebraic derivation "buried" the negative value of t2' and it was not evident when you just use the differences of the x's and t's. When we approached it in two steps, we found it out again, if we looked for it. Now we are dealing with coordinates in space-time and because of the placing the origin of O' on top of the origin of O, we have a negative number for t2' but it is all relative, hence, no harm no foul.

Since this not a trip but a rod, we can have two different but simultaneous events, and they are simultaneous because they are being done at the same time in frame O. If one were himself or herself in O' we would "see" the measurement at the front of of the rod being done 7.2 years (-7.2, 12, 0, 0) ahead of the measurement at the back end of the rod (0, 0, 0, 0).

In most texts I have seen, they gloss over all this middle men part of the calculations and just state (using the terminology of pc2-brazil and starthaus) L = L'/[tex]\gamma[/tex] which yields the same results and does not require delving into Minkowski space.
 
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  • #53
stevmg said:
In most texts I have seen, they gloss over all this middle men part of the calculations and just state (using the terminology of pc2-brazil and starthaus) L = L'/[tex]\gamma[/tex] which yields the same results and does not require delving into Minkowski space.

The standard texts are very simple, they start with the Lorentz transform:

[tex]x'=\gamma(x-vt)[/tex]
[tex]t'=\gamma(t-vx/c^2[/tex]

then, they calculate:[tex]dx'=\gamma(dx-vdt)[/tex]
[tex]dt'=\gamma(dt-vdx/c^2[/tex]

In order to calculate the length [tex]L'=dx'[/tex] as a function of the length [tex]L=dx[/tex]
the texts make use of the fact that [tex]dt'=0[/tex] (you must mark both ends of L' simultaneously in frame F'). This gives:

[tex]dt=vdx/c^2[/tex]

Substitute in the first equation and you will get:

[tex] L'=L/\gamma[/tex]

None of your the impossible to follow manipulations. For example:

Equation 2:
t2' = [tex]\gamma[/tex]*[t2 -vx2] = 1.25*[0 - (0.6)x2]
t2' = -1.25*0.6x2
t2' = -0.75x2

is not usable since [tex]t'_1=0[/tex] is DIFFERENT from your [tex]t'_2[/tex] above. The theory of measurement REQUIRES that you mark both ends of the rod simultaneously, i.e. [tex]t'_1=t'_2[/tex]. So, the fact that you obtained the correct result for [tex]L'[/tex] is purely accidental.
 
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  • #54
Posts 1 - 5 of this topic says the opposite of what you just stated above in post 53. In those earlier posts you stated that t1' does not equal t2' and you wanted t1 = t2 because we were measuring the result in the unprimed frame.

The answer of 9.6 ly is not accidental. It follows from the already proven L = L'/[tex]\gamma[/tex].

Remember, as per pc2-brazil, we were given (x2' - x1'. That's what pc2-brazil stated and you went along with. He wanted to use t1' = t2' but you changed that to t1 = t2 and stated that t1' could not equal t2' because of the relativity of simultaneity. Just reread those posts. I didn't write them, you and pc2-brazil did.
 
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  • #55
stevmg said:
Posts 1 - 5 of this topic says the opposite of what you just stated above in post 53. In those earlier posts you stated that t1' does not equal t2' and you wanted t1 = t2 because we were measuring the result in the unprimed frame.

If you want to measure [tex]x'_2-x'_1[/tex] you need to make [tex]t'_2=t'_1[/tex].
If you want to measure [tex]x_2-x_1[/tex] you need to make [tex]t_2=t_1[/tex].
I think I already told you this a few times.


Remember, as per pc2-brazil, we were given (x2' - x1'. That's what pc2-brazil stated and you went along with. He wanted to use t1' = t2' but you changed that to t1 = t2 and stated that t1' could not equal t2' because of the relativity of simultaneity. Just reread those posts. I didn't write them, you and pc2-brazil did.

At this rate , you'll never learn anything.
 
  • #56
Well, actually I have learned a lot.

Too bad that we are not in a classroom with a blackboard, where the give and take is quicker and sometimes the light bulb goes off sooner. Right now, you're right. I am stuck in neutral. But I can tell you this:

If you have a rod of length L' as measured in O' and with O' moving at v relative to O, by length contraction when you transform this to what an observer in O (unprimed frame) sees, he/she will see a rod of length L = L'/[tex]\gamma[/tex].

JesseM and DaleSpam went over that with me (as well as with many others) in the Einstein train thread. That isn't hard to understand. Dr. Einstein demonstrated that in a simplistic way (he was great at breaking things down to simple elements) in Section XII. "Rods and Clocks in motion" in Relativity.

If you want to have one more pass before you say the hell with me, consider below

"If you want to measure x2' - x1' you need to make t1' = t2'
If you want to measure x2 - x1 you need to make t1 = t2"

This is quoting what you have stated above several different times in the thread.

It appears that in the case that I presented, we are to apply the 12 ly (x2' - x1') to O' (because that is where it is "measured") and use t1' = t2' which would be zero. We would then transform this to O via Einstein-Lorentz and would wind up with an x1 and x2 which would be the length (L) in O. Are we on the same sheet of music? I know it seems redundant and beyond elemental but just answer the question. In other words, we "measured" L' and from that will calculate L.
 
  • #57
stevmg said:
It appears that in the case that I presented, we are to apply the 12 ly (x2' - x1') to O' (because that is where it is "measured") and use t1' = t2' which would be zero. We would then transform this to O via Einstein-Lorentz and would wind up with an x1 and x2 which would be the length (L) in O. Are we on the same sheet of music?

Nope. This is wrong. Remember the rule, in order to get a valid answer in O you need to measure [tex]x_2-x_1[/tex] for [tex]t_2=t_1[/tex]. When you "Lorentz transform" [tex]t'_2[/tex] and [tex]t'_1[/tex] into O, you will NOT get [tex]t_2=t_1[/tex], so you will not get a valid measurement. Why is this so, Steve?
 
  • #58
That is because of the relativity of simultaneity, i.e., when t2'=t1' in O', when these are transformed, the "corresponding t's" are not equal any longer. They are only equal in the original frame (O') because they were "set" that way by virtue of a measurement of the front and back of the rod being done together. The measurement of the rod in O' means that all elements from front to back are measured at the same time.

There's the "jump" where I am hung up. I comprehend the measurement in O' as pc2-brazil presented (x2' - x1' = L')

But I want to stop here and have you "OK" what I have said so far. If so, I will then proceed.
 
  • #59
stevmg said:
That is because of the relativity of simultaneity, i.e., when t2'=t1' in O', when these are transformed, the "corresponding t's" are not equal any longer. They are only equal in the original frame (O') because they were "set" that way by virtue of a measurement of the front and back of the rod being done together. The measurement of the rod in O' means that all elements from front to back are measured at the same time.

Yes, this is correct. Now you understand why I objected to your method?
 
  • #60
I will understand it more when I successfully complete the problem.

As I read pc2-brazil's opening statement (post 1, this thread) it appears that he knows L' (or x2' - x1') and, by consequence, t1' = t2' because he measured the position of the front of the rod (x2') at the same time (t2' = t1') he measured the position of the back of the rod (x1').

That is the core of my confusion: when you used the word "measure" it would seem that you mean "calculate." We are given x1', x2', t1' = t2' so we would not need to measure x2' - x1' therefore we would want to calculate x2 - x1 or L.

We would not get a "good" calculation of x2 - x1 unless t1 = t2. If I calculate t1 and t2 from the data given on x1', x2', t1' and t2', I will NOT get t1 = t2 because of this relativity of simultaneity.

At this point I will stop again, to wait for the "OK" on what I have just stated. So, let's make sure I have this correct so far.
 
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  • #61
stevmg said:
We would not get a "good" calculation of x2 - x1 unless t1 = t2. If I calculate t1 and t2 from the data given on x1', x2', t1' and t2', I will NOT get t1 = t2 because of this relativity of simultaneity.
Right. So you can EITHER calculate L as L'/gamma OR L' as L/\gamma.
 
  • #62
starthaus: Let's say I make the measurement of L from O and want to measure by which factor L is smaller than L', the proper length (length measured by O', according to which the measured object is at rest). Why can't I obtain this relation (which is L = L'/γ) by writing x'2 - x'1 with t2 = t1?
I still don't understand why this is wrong. This seems to be calculated like this very commonly. For example:
http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/tdil.html
 
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  • #63
pc2-brazil said:
starthaus: Let's say I make the measurement of L from O and want to measure by which factor L is smaller than L', the proper length (length measured by O', according to which the measured object is at rest). Why can't I obtain this relation (which is L = L'/γ) by writing x'2 - x'1 with t2 = t1?
I still don't understand why this is wrong.

Because the theory of measurement says that , in order to calculate the length of an objects in a frame, you need to mark its endpoints simultaneously in THAT particular frame.

This seems to be calculated like this very commonly. For example:
http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/tdil.html

It says quite clearly, that it calculates the length [tex]x_2-x_1[/tex] for [tex]t_2=t_1[/tex], exactly what I have been saying several times in this thread.
 
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  • #64
starthaus said:
It says quite clearly, that it calculates the length [tex]x_2-x_1[/tex] for [tex]t_2=t_1[/tex], exactly what I have been saying several times in this thread.
And also what I was trying to say.
If that in the site is written correctly, then what I wrote in the last phrase of post #14 is correct.
Unless I expressed myself badly. I want to measure x2 - x1 with t2 = t1, but start the resolution of the problem by writing x'2 - x'1 and substituting it for the Lorentz transformations instead of doing it the other way: writing x2 - x1. Then, I obtain L = L'/γ.
 
  • #65
pc2-brazil said:
And also what I was trying to say.
If that in the site is written correctly, then what I wrote in the last phrase of post #14 is correct.
Unless I expressed myself badly. I want to measure x2 - x1 with t2 = t1, but start the resolution of the problem by writing x'2 - x'1 and substituting it for the Lorentz transformations instead of doing it the other way: writing x2 - x1. Then, I obtain L = L'/γ.

ok, then
 
  • #66
Dr. Einstein, with very simple algebra and calculations proves what both of you (pc2-brazil and starthaus) are saying: L = L'/[tex]\gamma[/tex]. In his book, Relativity, Section XII "The Behaviour of Measuring Rods and Clocks in Motion" he puts his derivation in this format as opposed to L' = [tex]\gamma[/tex]L. If you assume that x1' and x2' are given in O' and x1' and x2' are fixed in O' and you "Lorentz" them to x1 and x2 in O and you do it in a way that pc2-brazil algebraically defines, you will wind up with t1 = t2 (because that's the way he set it up - to come out that way.) Thus, you are measuring x1 and x2 at he same time (simultaneously) in O. Because simultaneity is not preserved from different frames of reference, in O', the "corresponding t' s" are not equal to each other as they were in O. This is algebraically established in the second to last paragraph of this post. But that doesn't make any difference. Since x1' and x2' are fixed in O' as this was a given, the actual times of measurement of x1' and x2' in O' are immaterial to their measurements because these measurements never change in that frame of reference.

Final point, to establish that I do understand the derivation of L = L'/[tex]\gamma[/tex] or L' = [tex]\gamma[/tex]L:

x2'= [tex]\gamma[/tex][x2 - vt2]
x1'= [tex]\gamma[/tex][x1 - vt1]
x2' - x1' = L' = [tex]\gamma[/tex][x2 - x1 - (vt2 - vt1)]
but t2 = t1, therefore
x2' - x1' = L' = [tex]\gamma[/tex][x2 - x1 - (vt2 - vt2)] = [tex]\gamma[/tex](x2 - x1) = L
L' = [tex]\gamma[/tex]L
Q.E.D.

Just for the record:
t2' = [tex]\gamma[/tex](t2 - vx2)
t1' = [tex]\gamma[/tex](t1 - vx1)
but t2 = t1, therefore
t2' = [tex]\gamma[/tex](t2 - vx2)
t1' = [tex]\gamma[/tex](t2 - vx1)
t2' - t1' = [tex]\gamma[/tex][v(x1 - x2)] which is not zero.
This shows that t2' does not = t1'. Again, this is irrelevant as x1' and x2' never change with time in O' because this was stipulated as a given so the L' = [tex]\gamma[/tex]L relationship holds.

If I am wrong, please, please, please do NOT call me a dolt. I was born during the day, but not yesterday. Pardon any typos. I tried to clean them up but this is so damn cumbersome I may have missed a few.
 
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  • #67
To starthaus:

These two quotes answers the "why" one can use x1' and x2' in which t1' [tex]\neq[/tex] t2' (i.e, differing times when the rod is measured between front and back) for the calculation which t1 = t2 in S (or frame O in the pc2-brazil question.) Up until that point I couldn't make the "jump" and figure how you were still able to use the length of the rod in S' or L' as pc2-brazil stated it with its differing times of measurement of the front and back to calculate the length (L) in frame O in which the times of measurement of the front and back were the same.

stevmg said:
Back to Frame-Dragger:

If I do place a rod of certain length l0 in the moving frame S' which moves at a velocity of v to the right with respect to the stationary frame S and measure it in the stationary frame S at x1 and x2 simultaneously at t1 = t2, we get the length l0 = x2 - x1 according to the length contraction formula l0 = l/gamma. However, when we solve the simultaneous Lorentz equations for t1' and t2' in in S' which are the corresponding times for the t1 = t2 in S we note that t1' does not = t2[tex]\neq[/tex]' which means we measured the front and back of the rod at different times in S'.

Since the rod was stationary in S' it does not make a difference for l = x2' - x1' as both x2' and x1' are fixed in S' so that l will always be the same no matter when you measure the rod even if you measure the front and back at different times in that moving frame.

Is that logic correct? If so, this would justify the equation l0 = l/gamma

l = length in moving frame S'
l0 = length in resting frame S

jtbell said:
Yes, exactly so. Going the other way, if we measure the ends of the rod simultaneously in S' at t2' = t1', we similarly find that in S, t2 ≠ t1. This matters because the rod is not stationary in S.
 
  • #68
pc2-brazil said:
One end of the object is at x'1 x'2. Then, the length of the object in the primed reference frame is L' = x'2 - x'1.

Two questions:

Question 1:

What do you mean exactly by the sentence: "One end of the object is at x'1 x'2."

Question 2:

Should it not be the case, that x'2 > x'1?

PS. I followed the same approach as you did in the thread: Derivation of Proper Time and Proper Space.
 
  • #69
AdVen said:
Two questions:

Question 1:

What do you mean exactly by the sentence: "One end of the object is at x'1 x'2."

Should read one end of the object is at x'1 and the further end is at x'2

Question 2:

Should it not be the case, that x'2 > x'1?

Yes, that is correct.

PS. I followed the same approach as you did in the thread: Derivation of Proper Time and Proper Space.


Where have you been? I wrote that weeks ago! Not harassing you - just asking.
 
  • #70
starthaus said:
The math that you wrote below contradicts your above statement.





When you write x'2 - x'1 it means that you are measuring in the primed frame.



One more time, L' = γL is wrong. If you did things correctly you should have gotten L' = L/γ


If L' = L/γ then one would expect L = γ L'.
 

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