THE EHRENFEST PARADOX



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Topic: Science > Physics
User: "Pentcho Valev"
Date: 21 Sep 2006 11:08:33 AM
Object: THE EHRENFEST PARADOX
By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:
1. Ehrenfest: The ratio is smaller than pi.
2. Einstein: The ratio is greater than pi.
3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.
4. The rest of the scientific world: Who cares.
Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.
Pentcho Valev
.

User: "harry"

Title: Re: THE EHRENFEST PARADOX 22 Sep 2006 04:52:55 AM
"Pentcho Valev" <pvalev@yahoo.com> wrote in message
news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

"The" of 1 differs completely from "The" of 2...

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

Probably a third "The".

4. The rest of the scientific world: Who cares.

Indeed it doesn't matter.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

You are confused but -contrary to other occasions- here it's not entirely
your fault, as much of the literature about these matters is confused.
Harald

Pentcho Valev

.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 22 Sep 2006 05:17:30 AM
"harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
news:1158918775_15@sicinfo3.epfl.ch...
|
| "Pentcho Valev" <pvalev@yahoo.com> wrote in message
| news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...
| > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > measuring rods laid out along the rim of a rotating disc are Lorentz
| > contracted whereas those laid out along the radius are not and
| > therefore the ratio of the circumference and the diameter, as judged by
| > a non-rotating observer, is no longer pi. The problem is usually
| > referred to as the Ehrenfest paradox and has four solutions:
| >
| > 1. Ehrenfest: The ratio is smaller than pi.
| >
| > 2. Einstein: The ratio is greater than pi.
|
| "The" of 1 differs completely from "The" of 2...
So what are you whining about?
x' differs completely from x'
http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
van lintel = confused fuckwit
.
User: "harry"

Title: Re: THE EHRENFEST PARADOX 27 Sep 2006 06:57:12 AM
"Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
news:_KOQg.32797$wg.15945@fe1.news.blueyonder.co.uk...


"harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
news:1158918775_15@sicinfo3.epfl.ch...
|
| "Pentcho Valev" <pvalev@yahoo.com> wrote in message
| news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...
| > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > measuring rods laid out along the rim of a rotating disc are Lorentz
| > contracted whereas those laid out along the radius are not and
| > therefore the ratio of the circumference and the diameter, as judged
by
| > a non-rotating observer, is no longer pi. The problem is usually
| > referred to as the Ehrenfest paradox and has four solutions:
| >
| > 1. Ehrenfest: The ratio is smaller than pi.
| >
| > 2. Einstein: The ratio is greater than pi.
|
| "The" of 1 differs completely from "The" of 2...

So what are you whining about?
x' differs completely from x'
http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm

That's a great animation except for the train stretching and compressing;
it's certainly wrong but too confusing to point out what exactly. It would
be much better to have two animations, one above the other, of how it looks
like inside the train and how it looks like along the track.
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 27 Sep 2006 07:37:55 AM
"harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
news:1159358232_57@sicinfo3.epfl.ch...
|
| "Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
| news:_KOQg.32797$wg.15945@fe1.news.blueyonder.co.uk...
| >
| > "harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
| > news:1158918775_15@sicinfo3.epfl.ch...
| > |
| > | "Pentcho Valev" <pvalev@yahoo.com> wrote in message
| > | news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...
| > | > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > | > measuring rods laid out along the rim of a rotating disc are Lorentz
| > | > contracted whereas those laid out along the radius are not and
| > | > therefore the ratio of the circumference and the diameter, as judged
| > by
| > | > a non-rotating observer, is no longer pi. The problem is usually
| > | > referred to as the Ehrenfest paradox and has four solutions:
| > | >
| > | > 1. Ehrenfest: The ratio is smaller than pi.
| > | >
| > | > 2. Einstein: The ratio is greater than pi.
| > |
| > | "The" of 1 differs completely from "The" of 2...
| >
| > So what are you whining about?
| > x' differs completely from x'
| > http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
|
| That's a great animation except for the train stretching and compressing;
That's the Lorentz contraction. You believe in that, it's the word of
of the prophet, Holy Einstein the Great.
300,000,000 m/s divided by 60 meters = 5,000,000 metres/sec, or 5
metres/microsecond.
Each car is 60 metres long.
The speed of light is 5 units (cars) a microsecond.
20/4 = 5 units/microsecond, each car shrinks to 20 metres.
80/16 = 5 units /microsecond, each car stretches to 80 meters.
It depends which way the laser pointer is aimed, of course.
Try it out. Get on a train with a laser pointer.
Half of 100 = 80, the other half is 20.-- Einstein math.
| it's certainly wrong but too confusing to point out what exactly.
The speed of light is exactly the same along the fence as it is along the
train.
No confused fuckwit relativist should ever say it is wrong, you are
denying your own religion.
| It would
| be much better to have two animations, one above the other, of how it
looks
| like inside the train and how it looks like along the track.
Go ahead, I'm not stopping you. <shrug>
Just make sure the speed of light is the same in all inertial frames of
reference.
Everyone knows worms use peristalsis, so do your intestines.
Trains do as well when you shine a light on them, Einstein said so.
Androcles
.
User: "harry"

Title: Re: THE EHRENFEST PARADOX 29 Sep 2006 09:38:38 AM
"Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
news:DguSg.45831$aP3.15761@fe3.news.blueyonder.co.uk...


"harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
news:1159358232_57@sicinfo3.epfl.ch...
|
| "Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
| news:_KOQg.32797$wg.15945@fe1.news.blueyonder.co.uk...
| >
| > "harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
| > news:1158918775_15@sicinfo3.epfl.ch...
| > |
| > | "Pentcho Valev" <pvalev@yahoo.com> wrote in message
| > | news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...
| > | > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > | > measuring rods laid out along the rim of a rotating disc are
Lorentz
| > | > contracted whereas those laid out along the radius are not and
| > | > therefore the ratio of the circumference and the diameter, as
judged
| > by
| > | > a non-rotating observer, is no longer pi. The problem is usually
| > | > referred to as the Ehrenfest paradox and has four solutions:
| > | >
| > | > 1. Ehrenfest: The ratio is smaller than pi.
| > | >
| > | > 2. Einstein: The ratio is greater than pi.
| > |
| > | "The" of 1 differs completely from "The" of 2...
| >
| > So what are you whining about?
| > x' differs completely from x'
| > http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
|
| That's a great animation except for the train stretching and
compressing;

That's the Lorentz contraction. You believe in that, it's the word of
of the prophet, Holy Einstein the Great.

300,000,000 m/s divided by 60 meters = 5,000,000 metres/sec, or 5
metres/microsecond.
Each car is 60 metres long.
The speed of light is 5 units (cars) a microsecond.


20/4 = 5 units/microsecond, each car shrinks to 20 metres.
80/16 = 5 units /microsecond, each car stretches to 80 meters.
It depends which way the laser pointer is aimed, of course.
Try it out. Get on a train with a laser pointer.

There *is* no stretching. But to make that clear, two animations will be
necessary as I suggested below.
Harald

Half of 100 = 80, the other half is 20.-- Einstein math.


| it's certainly wrong but too confusing to point out what exactly.

The speed of light is exactly the same along the fence as it is along the
train.
No confused fuckwit relativist should ever say it is wrong, you are
denying your own religion.


| It would
| be much better to have two animations, one above the other, of how it
looks
| like inside the train and how it looks like along the track.

Go ahead, I'm not stopping you. <shrug>
Just make sure the speed of light is the same in all inertial frames of
reference.
Everyone knows worms use peristalsis, so do your intestines.
Trains do as well when you shine a light on them, Einstein said so.
Androcles



.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 29 Sep 2006 11:04:53 AM
"harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
news:1159540718_89@sicinfo3.epfl.ch...
|
| "Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
| news:DguSg.45831$aP3.15761@fe3.news.blueyonder.co.uk...
| >
| > "harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
| > news:1159358232_57@sicinfo3.epfl.ch...
| > |
| > | "Sorcerer" <Headmaster@hogwarts.physics_b> wrote in message
| > | news:_KOQg.32797$wg.15945@fe1.news.blueyonder.co.uk...
| > | >
| > | > "harry" <harald.vanlintelButNotThis@epfl.ch> wrote in message
| > | > news:1158918775_15@sicinfo3.epfl.ch...
| > | > |
| > | > | "Pentcho Valev" <pvalev@yahoo.com> wrote in message
| > | > | news:1158854913.279813.110320@m73g2000cwd.googlegroups.com...
| > | > | > By the end of Chapter 23 in his "Relativity" Einstein claims
that
| > | > | > measuring rods laid out along the rim of a rotating disc are
| > Lorentz
| > | > | > contracted whereas those laid out along the radius are not and
| > | > | > therefore the ratio of the circumference and the diameter, as
| > judged
| > | > by
| > | > | > a non-rotating observer, is no longer pi. The problem is usually
| > | > | > referred to as the Ehrenfest paradox and has four solutions:
| > | > | >
| > | > | > 1. Ehrenfest: The ratio is smaller than pi.
| > | > | >
| > | > | > 2. Einstein: The ratio is greater than pi.
| > | > |
| > | > | "The" of 1 differs completely from "The" of 2...
| > | >
| > | > So what are you whining about?
| > | > x' differs completely from x'
| > | > http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
| > |
| > | That's a great animation except for the train stretching and
| > compressing;
| >
| > That's the Lorentz contraction. You believe in that, it's the word of
| > of the prophet, Holy Einstein the Great.
| >
| > 300,000,000 m/s divided by 60 meters = 5,000,000 metres/sec, or 5
| > metres/microsecond.
| > Each car is 60 metres long.
| > The speed of light is 5 units (cars) a microsecond.
| >
| >
| > 20/4 = 5 units/microsecond, each car shrinks to 20 metres.
| > 80/16 = 5 units /microsecond, each car stretches to 80 meters.
| > It depends which way the laser pointer is aimed, of course.
| > Try it out. Get on a train with a laser pointer.
|
| There *is* no stretching.
Oh, so you don't believe in the cuckoo misformation!
Too bad, the Lord Einstein will be very disappointed in you.
You must have faith, my son.
Say three Hail Aethers for your penance.
Hail Aether,
Full of Light,
Einstein is with thee.
Blessed art thou among absolute frames of reference,
and blessed is the fruit of thy tomb, Lorentz Transform.
Holy Aether,
Daughter of Lunacy,
prey on us morons now,
and at the dilated hour of death.
Father Androcles
.






User: ""

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 11:42:03 AM
Pencho, you raise an interesting but rather obscure point.
First, to the best of my knowledge Pi has no real significance in a
relativistic framework, nor have many people actually considered the
mechanical issue of a rotating disk at edge velocities approaching 'C'.
Still it is an interesting thought experiment.
It is important to realize that Pi is first fallout from the solution
of various mathematics equations, and and that it is the observed
relationship between the diameter and circumference is little more than
an interesting coincidence -- although it could be more important than
simply an empirical ratio.
Pi, like "e", is one of those magic numbers that pop up in mathematics.
Both are significant since we cannot place an exact value on either.
With the advent of computrers, the value of both Pi and e have been
computed to many thousands of decimal places, but a precise value for
either appears impossible to obtain. Perhaps this is because the
Creator like to throw us a little curve once in a while to keep our
respective egos in check. :-) Still, I find this most curious.
Getting back to the spinning wheel. While an interesting though
experiment, and exact solution taking relativity into account is quite
difficult from an analytical standpoint. One problem in doing this is
that the tangental velocity of all portions of the disk is related by
Pi to its angular velocity, and if Pi is not constant but varies with
velocity, that's a very nasty thing to model even with a computer. You
have to make assumptions, assumptions that you would prefer to have the
model tell you. We get into a chicken and egg situation very quickly.
I have to agree that the relativistic rotating wheel is an interesting
thing to think about, but a clear solution is so difficult to arrive
upon, that I am surprise that Einsten used in in one of his books,
because most of his illustrative models were so clear.
Harry C.
Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev

.
User: "harry"

Title: Re: THE EHRENFEST PARADOX 22 Sep 2006 05:10:16 AM
<hhc314@yahoo.com> wrote in message
news:1158856923.832513.255060@m7g2000cwm.googlegroups.com...

Pencho, you raise an interesting but rather obscure point.

First, to the best of my knowledge Pi has no real significance in a
relativistic framework, nor have many people actually considered the
mechanical issue of a rotating disk at edge velocities approaching 'C'.
Still it is an interesting thought experiment.

It is important to realize that Pi is first fallout from the solution
of various mathematics equations, and and that it is the observed
relationship between the diameter and circumference is little more than
an interesting coincidence -- although it could be more important than
simply an empirical ratio.

Pi, like "e", is one of those magic numbers that pop up in mathematics.
Both are significant since we cannot place an exact value on either.
With the advent of computrers, the value of both Pi and e have been
computed to many thousands of decimal places, but a precise value for
either appears impossible to obtain. Perhaps this is because the
Creator like to throw us a little curve once in a while to keep our
respective egos in check. :-) Still, I find this most curious.

Getting back to the spinning wheel. While an interesting though
experiment, and exact solution taking relativity into account is quite
difficult from an analytical standpoint. One problem in doing this is
that the tangental velocity of all portions of the disk is related by
Pi to its angular velocity, and if Pi is not constant but varies with
velocity, that's a very nasty thing to model even with a computer. You
have to make assumptions, assumptions that you would prefer to have the
model tell you. We get into a chicken and egg situation very quickly.

I have to agree that the relativistic rotating wheel is an interesting
thing to think about, but a clear solution is so difficult to arrive
upon, that I am surprise that Einsten used in in one of his books,
because most of his illustrative models were so clear.

Harry C.

Hi Harry, clear solutions *have* been arrived upon rather early, that's not
the problem. Regretfully too many confusing papers have been written about
significantly different problems that were suggested to be the same one.
Cheers,
Harald

Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev


.

User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 11:55:27 AM
<hhc314@yahoo.com> wrote in message
news:1158856923.832513.255060@m7g2000cwm.googlegroups.com...
| Pencho, you raise an interesting but rather obscure point.
|
| First, to the best of my knowledge Pi has no real significance in a
| relativistic framework,
http://www.fourmilab.ch/etexts/einstein/specrel/www/figures/img107.gif
Update your knowledge.
To the best of your knowledge, cos(pi/2) = 0, even it Einstein's
fuckwittery.
Engage brain before opening mouth.
.


User: "Phil"

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 01:04:14 PM
Pentcho Valev wrote:


Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity . . .

This is Einstein's solution? Really doesn't make sense that it would
be. If the measuring rod is contracted (to the non-rotating observer),
so is the outer edge of the disc. I doubt Einstein would have drawn
the conclusion you have reported here.
Here is another way of looking at it. There is a football field in a
spaceship and a yard stick. Whether Lorentz contracted or not, the
yardstick is alway 1/100 the length of the playing part of the field.

. . . and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev

That has to be nonsense. To the non rotating observer, and the radius
of constant value, the faster the disc spins, the less time required
for a mark to make a complete cycle.
Phil
.

User: "Igor"

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 01:05:14 PM
Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev

Is the ratio of the perimeter of an ellipse to either the major or
minor axis equal to pi?
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 01:56:00 PM
"Igor" <thoovler@excite.com> wrote in message
news:1158861914.183188.254170@m73g2000cwd.googlegroups.com...
|
| Pentcho Valev wrote:
| > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > measuring rods laid out along the rim of a rotating disc are Lorentz
| > contracted whereas those laid out along the radius are not and
| > therefore the ratio of the circumference and the diameter, as judged by
| > a non-rotating observer, is no longer pi. The problem is usually
| > referred to as the Ehrenfest paradox and has four solutions:
| >
| > 1. Ehrenfest: The ratio is smaller than pi.
| >
| > 2. Einstein: The ratio is greater than pi.
| >
| > 3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
| > pi.
| >
| > 4. The rest of the scientific world: Who cares.
| >
| > Einstein's solution is the most breathtaking: as the linear speed of
| > the periphery approaches the speed of light, the length of the
| > circumference approaches infinity and therefore the non-rotating
| > observer will never live long enough to see a mark on the periphery two
| > times.
| >
| > Pentcho Valev
|
| Is the ratio of the perimeter of an ellipse to either the major or
| minor axis equal to pi?
No, it's greater than pi for the minor axis and less than pi for the
major axis.
For all ellipses with eccentricity=1 the minor axis is zero miles, inches
centimetres or microns.
The man said a rotating disc, not an ellipse, square, triangle,
polygon, sphere or dodecahedron. DISC!
Did you have a point to make, stupid illiterate fuckwit troll?
Androcles.
.


User: ""

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 08:24:01 PM
Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev

xxein: None of the above. I did not investigate 3. If there is
something in there that is pertinent to my reply, then please post back
to me.
But let's look at spokes on a wheel. How fast can the spokes go as
they approach the periphery (circumference)? Don't they bend and
increase in distance from the hub? Wouldn't the radial distance match
circumference wrt pi?
Just want to know if you thought of that.
Thx.
.
User: "Stamenin"

Title: Re: THE EHRENFEST PARADOX 22 Sep 2006 12:47:14 AM
wrote:

Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the

I thik that Einstein forgot that the Lorentz transformation is valid
only for a right line motion.

circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

Pentcho Valev


xxein: None of the above. I did not investigate 3. If there is
something in there that is pertinent to my reply, then please post back
to me.

But let's look at spokes on a wheel. How fast can the spokes go as
they approach the periphery (circumference)? Don't they bend and
increase in distance from the hub? Wouldn't the radial distance match
circumference wrt pi?

Just want to know if you thought of that.

Thx.

.


User: "Sue..."

Title: Re: THE EHRENFEST PARADOX 21 Sep 2006 11:38:24 AM
Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.

http://www.bartleby.com/173/23.html
It is not an easy read but seem to suggest the light path from
the rim to hub is affected by
"an effect of inertia (centrifugal force)"
Right or wrong, it seems consistant with Schwarchild's
solution with ~falling light particles~ .
If two wrongs make a right I suppose the answer is
<< 4. The rest of the scientific world: Who cares.>>
You can put it in the same circular file with the
train and embankment story to keep it company
and then go check some maths.
Sue...


Pentcho Valev

.
User: "RP"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 11:22:17 AM
Sue... wrote:

Pentcho Valev wrote:

By the end of Chapter 23 in his "Relativity" Einstein claims that
measuring rods laid out along the rim of a rotating disc are Lorentz
contracted whereas those laid out along the radius are not and
therefore the ratio of the circumference and the diameter, as judged by
a non-rotating observer, is no longer pi. The problem is usually
referred to as the Ehrenfest paradox and has four solutions:

1. Ehrenfest: The ratio is smaller than pi.

2. Einstein: The ratio is greater than pi.

3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
pi.

4. The rest of the scientific world: Who cares.

Einstein's solution is the most breathtaking: as the linear speed of
the periphery approaches the speed of light, the length of the
circumference approaches infinity and therefore the non-rotating
observer will never live long enough to see a mark on the periphery two
times.


http://www.bartleby.com/173/23.html

It is not an easy read but seem to suggest the light path from
the rim to hub is affected by

"an effect of inertia (centrifugal force)"

Right or wrong, it seems consistant with Schwarchild's
solution with ~falling light particles~ .

If two wrongs make a right I suppose the answer is

<< 4. The rest of the scientific world: Who cares.>>

You can put it in the same circular file with the
train and embankment story to keep it company
and then go check some maths.

Sue...

That entire section is pretty sad. If the rotating observer states that
there is a gravitational field, then how does he account for the
reversing of its direction wrt any masses not in contact with the disc.
Suppose there is a mass that is at rest suspended over his head. From
his FoR that mass is in a circular orbit about the center of the disc,
and must therefore be experiencing a gravitational force acting toward
the center of the disc, whereas the same field is pushing him away from
the center of the disk. Absurd.
He need only drop a baseball in that field to find out that it is a
fictitious force. He will quickly discover that the only force acting
on him was a centripetal inertial force due to his accelleration, and
that he must therefore be actually accellerating wrt other masses in
the surrounding space which are themselves not located in gravitational
field.
The clock ticking rate offset can be derived perfectly in terms of the
lorentz transform. It is just the special relativistic ticking rate
offset due to its relative velocity. If we assume that it is a
gravitational ticking rate offset, then we must first dispose of the
special relatisitic offset, or else keep in the forefront of the
argument that these are one and the same ticking rate offsets with two
alternate explanations. If we then invoke the equivalence principle, we
should then be justified in ascribing the ticking rate offset of a
clock at rest on a real gravitating body to the special relativistic
ticking rate offset due to the relative motion of the clock wrt the
observer. This scheme won't work for obvious reasons, namely that the
clock is at rest wrt our FoR. Thus it would seem that the equivalence
principle doesn't commute, which I think is contradictory to the term
"equivalency" and thus in turn to the equivalence principle.
It's nonsense. The primary problem with most of Einsein's arguments is
that nature doesn't give a damn about frames of reference, they are
irrellevant to its workings, being nothing more than a contemplative
perspective of the universe.
Richard Perry
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 11:36:22 AM
"RP" <no_mail_no_spam@yahoo.com> wrote in message
news:1159114936.965542.193380@k70g2000cwa.googlegroups.com...
|
| Sue... wrote:
| > Pentcho Valev wrote:
| > > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > > measuring rods laid out along the rim of a rotating disc are Lorentz
| > > contracted whereas those laid out along the radius are not and
| > > therefore the ratio of the circumference and the diameter, as judged
by
| > > a non-rotating observer, is no longer pi. The problem is usually
| > > referred to as the Ehrenfest paradox and has four solutions:
| > >
| > > 1. Ehrenfest: The ratio is smaller than pi.
| > >
| > > 2. Einstein: The ratio is greater than pi.
| > >
| > > 3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
| > > pi.
| > >
| > > 4. The rest of the scientific world: Who cares.
| > >
| > > Einstein's solution is the most breathtaking: as the linear speed of
| > > the periphery approaches the speed of light, the length of the
| > > circumference approaches infinity and therefore the non-rotating
| > > observer will never live long enough to see a mark on the periphery
two
| > > times.
| >
| > http://www.bartleby.com/173/23.html
| >
| > It is not an easy read but seem to suggest the light path from
| > the rim to hub is affected by
| >
| > "an effect of inertia (centrifugal force)"
| >
| > Right or wrong, it seems consistant with Schwarchild's
| > solution with ~falling light particles~ .
| >
| > If two wrongs make a right I suppose the answer is
| >
| > << 4. The rest of the scientific world: Who cares.>>
| >
| > You can put it in the same circular file with the
| > train and embankment story to keep it company
| > and then go check some maths.
| >
| > Sue...
|
| That entire section is pretty sad. If the rotating observer states that
| there is a gravitational field, then how does he account for the
| reversing of its direction wrt any masses not in contact with the disc.
| Suppose there is a mass that is at rest suspended over his head. From
| his FoR that mass is in a circular orbit about the center of the disc,
| and must therefore be experiencing a gravitational force acting toward
| the center of the disc, whereas the same field is pushing him away from
| the center of the disk. Absurd.
| He need only drop a baseball in that field to find out that it is a
| fictitious force. He will quickly discover that the only force acting
| on him was a centripetal inertial force due to his accelleration, and
| that he must therefore be actually accellerating wrt other masses in
| the surrounding space which are themselves not located in gravitational
| field.
|
| The clock ticking rate offset can be derived perfectly in terms of the
| lorentz transform. It is just the special relativistic ticking rate
| offset due to its relative velocity. If we assume that it is a
| gravitational ticking rate offset, then we must first dispose of the
| special relatisitic offset, or else keep in the forefront of the
| argument that these are one and the same ticking rate offsets with two
| alternate explanations. If we then invoke the equivalence principle, we
| should then be justified in ascribing the ticking rate offset of a
| clock at rest on a real gravitating body to the special relativistic
| ticking rate offset due to the relative motion of the clock wrt the
| observer. This scheme won't work for obvious reasons, namely that the
| clock is at rest wrt our FoR. Thus it would seem that the equivalence
| principle doesn't commute, which I think is contradictory to the term
| "equivalency" and thus in turn to the equivalence principle.
|
| It's nonsense. The primary problem with most of Einsein's arguments is
| that nature doesn't give a damn about frames of reference, they are
| irrellevant to its workings, being nothing more than a contemplative
| perspective of the universe.
|
| Richard Perry
Einstein did not know what a half is. How sad is that?
http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
Androcles
.
User: "RP"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 12:41:08 PM
Sorcerer wrote:

"RP" <no_mail_no_spam@yahoo.com> wrote in message
news:1159114936.965542.193380@k70g2000cwa.googlegroups.com...
|
| Sue... wrote:
| > Pentcho Valev wrote:
| > > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > > measuring rods laid out along the rim of a rotating disc are Lorentz
| > > contracted whereas those laid out along the radius are not and
| > > therefore the ratio of the circumference and the diameter, as judged
by
| > > a non-rotating observer, is no longer pi. The problem is usually
| > > referred to as the Ehrenfest paradox and has four solutions:
| > >
| > > 1. Ehrenfest: The ratio is smaller than pi.
| > >
| > > 2. Einstein: The ratio is greater than pi.
| > >
| > > 3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is equal to
| > > pi.
| > >
| > > 4. The rest of the scientific world: Who cares.
| > >
| > > Einstein's solution is the most breathtaking: as the linear speed of
| > > the periphery approaches the speed of light, the length of the
| > > circumference approaches infinity and therefore the non-rotating
| > > observer will never live long enough to see a mark on the periphery
two
| > > times.
| >
| > http://www.bartleby.com/173/23.html
| >
| > It is not an easy read but seem to suggest the light path from
| > the rim to hub is affected by
| >
| > "an effect of inertia (centrifugal force)"
| >
| > Right or wrong, it seems consistant with Schwarchild's
| > solution with ~falling light particles~ .
| >
| > If two wrongs make a right I suppose the answer is
| >
| > << 4. The rest of the scientific world: Who cares.>>
| >
| > You can put it in the same circular file with the
| > train and embankment story to keep it company
| > and then go check some maths.
| >
| > Sue...
|
| That entire section is pretty sad. If the rotating observer states that
| there is a gravitational field, then how does he account for the
| reversing of its direction wrt any masses not in contact with the disc.
| Suppose there is a mass that is at rest suspended over his head. From
| his FoR that mass is in a circular orbit about the center of the disc,
| and must therefore be experiencing a gravitational force acting toward
| the center of the disc, whereas the same field is pushing him away from
| the center of the disk. Absurd.
| He need only drop a baseball in that field to find out that it is a
| fictitious force. He will quickly discover that the only force acting
| on him was a centripetal inertial force due to his accelleration, and
| that he must therefore be actually accellerating wrt other masses in
| the surrounding space which are themselves not located in gravitational
| field.
|
| The clock ticking rate offset can be derived perfectly in terms of the
| lorentz transform. It is just the special relativistic ticking rate
| offset due to its relative velocity. If we assume that it is a
| gravitational ticking rate offset, then we must first dispose of the
| special relatisitic offset, or else keep in the forefront of the
| argument that these are one and the same ticking rate offsets with two
| alternate explanations. If we then invoke the equivalence principle, we
| should then be justified in ascribing the ticking rate offset of a
| clock at rest on a real gravitating body to the special relativistic
| ticking rate offset due to the relative motion of the clock wrt the
| observer. This scheme won't work for obvious reasons, namely that the
| clock is at rest wrt our FoR. Thus it would seem that the equivalence
| principle doesn't commute, which I think is contradictory to the term
| "equivalency" and thus in turn to the equivalence principle.
|
| It's nonsense. The primary problem with most of Einsein's arguments is
| that nature doesn't give a damn about frames of reference, they are
| irrellevant to its workings, being nothing more than a contemplative
| perspective of the universe.
|
| Richard Perry

Einstein did not know what a half is. How sad is that?
http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
Androcles

The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.
Yes, I know, they look the same, but they are not.
The first view, that of Einstein, is that reality is frame dependent,
ie. the B field in one frame is very real, and the absense of this
field wrt another observer is of no consequence, since their realities
simply differer. While admitting that the B and E fields are just
perspectives of a single em field, this overlooks the fact that the E
field of a static charge cannot be transformed to a B field by any
means, yet no such invariant version of the B field exists. There are
no magnetic monopoles. His is actually the many-worlds interpreation-a
different set of inputs leading to the same objective events, but this
approach does encounter a few obvious glitches.
The second view, mine and Newton's, is that frames of reference are
eqquivalent because they are all equally irrelevant. In my view there
is no B field wrt any frame, except as a pure mathematical abstraction.
All real things are objective, including the processes that lead up to
them, they themselves being objective outcomes of events that preceeded
them.
The idea that an observer has the right to consider himself at rest,
though true, is irrelevant, because it is the motion of particles wrt
each other that matters. Thier motions wrt you is completely irrelevant
to the interaction that occurs. It would occur precisely the same
whether or not you exist.
Thus the real problem here is an ontological one, namely the fact that
in Einstien's view the universe is geo-centric, or better ego-centric.
He establishes the observer as God, and the universe must conform to
his views. I suggest a humbler approach, namely, that the universe is
the master, and we must conform our views to it.
Richard Perry
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 03:11:25 PM
"RP" <no_mail_no_spam@yahoo.com> wrote in message
news:1159119668.777035.245320@m7g2000cwm.googlegroups.com...
|
| Sorcerer wrote:
| > "RP" <no_mail_no_spam@yahoo.com> wrote in message
| > news:1159114936.965542.193380@k70g2000cwa.googlegroups.com...
| > |
| > | Sue... wrote:
| > | > Pentcho Valev wrote:
| > | > > By the end of Chapter 23 in his "Relativity" Einstein claims that
| > | > > measuring rods laid out along the rim of a rotating disc are
Lorentz
| > | > > contracted whereas those laid out along the radius are not and
| > | > > therefore the ratio of the circumference and the diameter, as
judged
| > by
| > | > > a non-rotating observer, is no longer pi. The problem is usually
| > | > > referred to as the Ehrenfest paradox and has four solutions:
| > | > >
| > | > > 1. Ehrenfest: The ratio is smaller than pi.
| > | > >
| > | > > 2. Einstein: The ratio is greater than pi.
| > | > >
| > | > > 3. M. Strauss (Int.J.Theor.Phys. 11, 107, 1974): The ratio is
equal to
| > | > > pi.
| > | > >
| > | > > 4. The rest of the scientific world: Who cares.
| > | > >
| > | > > Einstein's solution is the most breathtaking: as the linear speed
of
| > | > > the periphery approaches the speed of light, the length of the
| > | > > circumference approaches infinity and therefore the non-rotating
| > | > > observer will never live long enough to see a mark on the
periphery
| > two
| > | > > times.
| > | >
| > | > http://www.bartleby.com/173/23.html
| > | >
| > | > It is not an easy read but seem to suggest the light path from
| > | > the rim to hub is affected by
| > | >
| > | > "an effect of inertia (centrifugal force)"
| > | >
| > | > Right or wrong, it seems consistant with Schwarchild's
| > | > solution with ~falling light particles~ .
| > | >
| > | > If two wrongs make a right I suppose the answer is
| > | >
| > | > << 4. The rest of the scientific world: Who cares.>>
| > | >
| > | > You can put it in the same circular file with the
| > | > train and embankment story to keep it company
| > | > and then go check some maths.
| > | >
| > | > Sue...
| > |
| > | That entire section is pretty sad. If the rotating observer states
that
| > | there is a gravitational field, then how does he account for the
| > | reversing of its direction wrt any masses not in contact with the
disc.
| > | Suppose there is a mass that is at rest suspended over his head. From
| > | his FoR that mass is in a circular orbit about the center of the disc,
| > | and must therefore be experiencing a gravitational force acting toward
| > | the center of the disc, whereas the same field is pushing him away
from
| > | the center of the disk. Absurd.
| > | He need only drop a baseball in that field to find out that it is a
| > | fictitious force. He will quickly discover that the only force acting
| > | on him was a centripetal inertial force due to his accelleration, and
| > | that he must therefore be actually accellerating wrt other masses in
| > | the surrounding space which are themselves not located in
gravitational
| > | field.
| > |
| > | The clock ticking rate offset can be derived perfectly in terms of the
| > | lorentz transform. It is just the special relativistic ticking rate
| > | offset due to its relative velocity. If we assume that it is a
| > | gravitational ticking rate offset, then we must first dispose of the
| > | special relatisitic offset, or else keep in the forefront of the
| > | argument that these are one and the same ticking rate offsets with two
| > | alternate explanations. If we then invoke the equivalence principle,
we
| > | should then be justified in ascribing the ticking rate offset of a
| > | clock at rest on a real gravitating body to the special relativistic
| > | ticking rate offset due to the relative motion of the clock wrt the
| > | observer. This scheme won't work for obvious reasons, namely that the
| > | clock is at rest wrt our FoR. Thus it would seem that the equivalence
| > | principle doesn't commute, which I think is contradictory to the term
| > | "equivalency" and thus in turn to the equivalence principle.
| > |
| > | It's nonsense. The primary problem with most of Einsein's arguments is
| > | that nature doesn't give a damn about frames of reference, they are
| > | irrellevant to its workings, being nothing more than a contemplative
| > | perspective of the universe.
| > |
| > | Richard Perry
| >
| > Einstein did not know what a half is. How sad is that?
| > http://www.androcles01.pwp.blueyonder.co.uk/Smart/Smart.htm
| > Androcles
|
| The principle of relativity can be stated in two ways:
| 1) All frames of reference are equivalent for the derivation of the
| laws of physics.
| 2) All frames of reference are equivalent for the derivation of the
| laws of physics.
|
| Yes, I know, they look the same, but they are not.
The principle of relativity can be stated in three ways:
3) "Examples of this sort":- "for example, the reciprocal electrodynamic
action of a magnet and a conductor." ...[insert caveat] ... will hereafter
be called the ``Principle of Relativity''.
Ref: http://www.fourmilab.ch/etexts/einstein/specrel/www/ pararagraphs 1
and 2.
You are right, they are not the same, a caveat is not the predicate of the
subject.
Why you should imagine they look the same, though, is a mystery only you can
answer.
A better example of the Principle of Relativity was given by Copernicus when
he announced the heliocentric universe.
|
| The first view, that of Einstein, is that reality is frame dependent,
| ie. the B field in one frame is very real, and the absense of this
| field wrt another observer is of no consequence, since their realities
| simply differer. While admitting that the B and E fields are just
| perspectives of a single em field, this overlooks the fact that the E
| field of a static charge cannot be transformed to a B field by any
| means, yet no such invariant version of the B field exists. There are
| no magnetic monopoles.
There are no electric monopoles.
Yes, that is what I said.
All electrical discharges are between poles.
| His is actually the many-worlds interpreation-a
| different set of inputs leading to the same objective events, but this
| approach does encounter a few obvious glitches.
|
| The second view, mine and Newton's, is that frames of reference are
| eqquivalent because they are all equally irrelevant.
FoR's are very relevant, the laws of physics change.
http://ww2010.atmos.uiuc.edu/(Gh)/guides/mtr/fw/gifs/coriolis.mov
LAW I.
Every body perseveres in its state of revolution, or of uniform motion in a
circular line, unless it is compelled to change that state by forces
impressed thereon.
LAW II.
The alteration of revolution is ever proportional to the radius of the
motive force impressed; and is made in the direction of the spiral line in
which that force is impressed.
LAW III.
To every action there is never an opposed or equal reaction; or the mutual
actions of two bodies upon each other are never equal.
I do not disagree with Newton, I simply have a different frame of reference.
| In my view there
Ah--- is your view from your frame of reference?
| is no B field wrt any frame, except as a pure mathematical abstraction.
| All real things are objective, including the processes that lead up to
| them, they themselves being objective outcomes of events that preceeded
| them.
|
| The idea that an observer has the right to consider himself at rest,
| though true, is irrelevant, because it is the motion of particles wrt
| each other that matters.
I have to disagree with you. Newton would also.
| Thier motions wrt you is completely irrelevant
| to the interaction that occurs. It would occur precisely the same
| whether or not you exist.
<shrug>
| Thus the real problem here is an ontological one, namely the fact that
| in Einstien's view the universe is geo-centric, or better ego-centric.
There I do agree. Einstein saw himself as a god.
| He establishes the observer as God, and the universe must conform to
| his views. I suggest a humbler approach, namely, that the universe is
| the master, and we must conform our views to it.
Agreed. "Be reasonable, see it my way".
| Richard Perry
IMO we should reduce the Principle of Relativity to an equation:
dx/dt = -dx'/dt and banish egocentricity from science (and politics).
In other words the background moves:
http://www.androcles01.pwp.blueyonder.co.uk/Catalina/mercedescatalina.gif
Androcles.
.

User: "Mike"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 01:35:11 PM
RP wrote:


The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.

Yes, I know, they look the same, but they are not.


Hello crank. FYI this is the principle of relativity:
"The laws of physics are the same in any inertial frame, regardless of
position or velocity"
http://casa.colorado.edu/~ajsh/sr/postulate.html
Bye crank
Mike


Richard Perry

.
User: "RP"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 01:56:25 PM
Mike wrote:

RP wrote:


The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.

Yes, I know, they look the same, but they are not.



Hello crank. FYI this is the principle of relativity:

"The laws of physics are the same in any inertial frame, regardless of
position or velocity"

http://casa.colorado.edu/~ajsh/sr/postulate.html

Bye crank

Mike

Don't be a moron. That is the "restricted principle of relativity".
Try this,
"[...] In contrast to this we wish to understand by the "general
principle of
relativity" the following statement : All bodies of reference K, K1,
etc., are equivalent for the description of natural phenomena
(formulation of the general laws of nature), whatever may be their
state of motion." --Albert Einstein, "Relativity: The General and
Special Theory"
Dover Press
Adios moron. You've stepped in your own ***** once again. One would
think you'd learn something after smelling the stink that follows you
around.
Richard Perry
.

User: "RP"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 01:58:12 PM
Mike wrote:

RP wrote:


The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.

Yes, I know, they look the same, but they are not.



Hello crank. FYI this is the principle of relativity:

"The laws of physics are the same in any inertial frame, regardless of
position or velocity"

http://casa.colorado.edu/~ajsh/sr/postulate.html

Bye crank

Mike

Don't be a moron. That is the "restricted principle of relativity".
Try this,
"[...] In contrast to this we wish to understand by the "general
principle of
relativity" the following statement : All bodies of reference K, K1,
etc., are equivalent for the description of natural phenomena
(formulation of the general laws of nature), whatever may be their
state of motion." --Albert Einstein, "Relativity: The Special and
General Theory"
Adios moron. You've stepped in your own ***** once again. One would
think you'd learn something after smelling the stink that follows you
around.
Richard Perry
.
User: "Mike"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 06:13:22 PM
RP wrote:

Mike wrote:

RP wrote:


The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.

Yes, I know, they look the same, but they are not.



Hello crank. FYI this is the principle of relativity:

"The laws of physics are the same in any inertial frame, regardless of
position or velocity"

http://casa.colorado.edu/~ajsh/sr/postulate.html

Bye crank

Mike


Don't be a moron. That is the "restricted principle of relativity".

There is no such thing as a "restricted" PoR. There is a weak and
strong PoR. In SR, the PoR says that all laws of physics are the same
in all globally inertial FoRs. In GR, an attempt is made to extend this
principle to ALL [moving] FoRs.


Try this,
"[...] In contrast to this we wish to understand by the "general
principle of
relativity" the following statement : All bodies of reference K, K1,
etc., are equivalent for the description of natural phenomena
(formulation of the general laws of nature), whatever may be their
state of motion." --Albert Einstein, "Relativity: The Special and
General Theory"

And this says what you think it says, that, in your words, "All frames
of reference are equivalent for the derivation of the laws of physics".
Do you understand the difference between Einstein's "formulation of
general laws of nature" and your "derivation of the laws of physics"?
I could try to explain to you but you are too
stoooooooooooooooooooooooooopid to learn it. Start by wondering what
"derivation" of a law of physics means.


Adios moron. You've stepped in your own ***** once again. One would
think you'd learn something after smelling the stink that follows you
around.

I do not read popular science books like you do, in which physicists
try to explain in layma's terms their theories.
Mike

Richard Perry

.
User: "RP"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 08:26:41 PM
Mike wrote:

RP wrote:

Mike wrote:

RP wrote:


The principle of relativity can be stated in two ways:
1) All frames of reference are equivalent for the derivation of the
laws of physics.
2) All frames of reference are equivalent for the derivation of the
laws of physics.

Yes, I know, they look the same, but they are not.



Hello crank. FYI this is the principle of relativity:

"The laws of physics are the same in any inertial frame, regardless of
position or velocity"

http://casa.colorado.edu/~ajsh/sr/postulate.html

Bye crank

Mike


Don't be a moron. That is the "restricted principle of relativity".



There is no such thing as a "restricted" PoR. There is a weak and
strong PoR. In SR, the PoR says that all laws of physics are the same
in all globally inertial FoRs. In GR, an attempt is made to extend this
principle to ALL [moving] FoRs.

Sigh...
"[...]
We advance a step farther in our generalisation when we express the
tenet thus: If, relative to K, K1 is a uniformly moving co-ordinate
system devoid of rotation, then natural phenomena run their course
with respect to K1 according to exactly the same general laws as with
respect to K. This statement is called the principle of relativity (in
the restricted sense).
Ok, you got me, its the "principle of relativity in the restricted
sense".


Try this,
"[...] In contrast to this we wish to understand by the "general
principle of
relativity" the following statement : All bodies of reference K, K1,
etc., are equivalent for the description of natural phenomena
(formulation of the general laws of nature), whatever may be their
state of motion." --Albert Einstein, "Relativity: The Special and
General Theory"


And this says what you think it says, that, in your words, "All frames
of reference are equivalent for the derivation of the laws of physics".


Do you understand the difference between Einstein's "formulation of
general laws of nature" and your "derivation of the laws of physics"?

I could try to explain to you but you are too
stoooooooooooooooooooooooooopid to learn it. Start by wondering what
"derivation" of a law of physics means.

Please explain the difference.
Here's the difference, we don't know what the laws of nature are, or we
wouldn't still be trying to find them. I said corretly "laws of
physics". I apologize for making the necessary correction. Seems a
pebble is a stumbling block for some.


Adios moron. You've stepped in your own ***** once again. One would
think you'd learn something after smelling the stink that follows you
around.


I do not read popular science books like you do, in which physicists
try to explain in layma's terms their theories.

Since it's his theory, I supose he should know better than you what to
call his premises.


Mike

What's your problem anyway? Do you think that Einstein himself didn't
make a few statements about existing theory of the negative sort? If
you'll read his "Ideas and Opinions", you might even wonder why some
government didn't have him removed. No kidding. He spoke his mind and
let the chips fall. He was just the sort of guy that I am in that
sense. I'm only sorry that you have little understanding of the process
called changing of the guards. It's never a tea party. If you don't
agree with a statement that's one thing. If your only intent is to
***** like a worn out old *****, then you can just gfys.
Richard Perry
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 25 Sep 2006 03:56:52 AM
"RP" <no_mail_no_spam@yahoo.com> wrote in message
news:1159147601.372727.131620@m7g2000cwm.googlegroups.com...
|
| Mike wrote:
| > RP wrote:
| > > Mike wrote:
| > > > RP wrote:
| > > > >
| > > > > The principle of relativity can be stated in two ways:
| > > > > 1) All frames of reference are equivalent for the derivation of
the
| > > > > laws of physics.
| > > > > 2) All frames of reference are equivalent for the derivation of
the
| > > > > laws of physics.
| > > > >
| > > > > Yes, I know, they look the same, but they are not.
| > > > >
| > > > >
| > > >
| > > > Hello crank. FYI this is the principle of relativity:
| > > >
| > > > "The laws of physics are the same in any inertial frame, regardless
of
| > > > position or velocity"
| > > >
| > > > http://casa.colorado.edu/~ajsh/sr/postulate.html
| > > >
| > > > Bye crank
| > > >
| > > > Mike
| > > >
| > >
| > > Don't be a moron. That is the "restricted principle of relativity".
| >
| >
| > There is no such thing as a "restricted" PoR. There is a weak and
| > strong PoR. In SR, the PoR says that all laws of physics are the same
| > in all globally inertial FoRs. In GR, an attempt is made to extend this
| > principle to ALL [moving] FoRs.
| >
|
| Sigh...
|
| "[...]
| We advance a step farther in our generalisation when we express the
| tenet thus: If, relative to K, K1 is a uniformly moving co-ordinate
| system devoid of rotation, then natural phenomena run their course
| with respect to K1 according to exactly the same general laws as with
| respect to K. This statement is called the principle of relativity (in
| the restricted sense).
|
| Ok, you got me, its the "principle of relativity in the restricted
| sense".
|
|
| > >
| > > Try this,
| > > "[...] In contrast to this we wish to understand by the "general
| > > principle of
| > > relativity" the following statement : All bodies of reference K, K1,
| > > etc., are equivalent for the description of natural phenomena
| > > (formulation of the general laws of nature), whatever may be their
| > > state of motion." --Albert Einstein, "Relativity: The Special and
| > > General Theory"
| >
| > And this says what you think it says, that, in your words, "All frames
| > of reference are equivalent for the derivation of the laws of physics".
| >
| >
| > Do you understand the difference between Einstein's "formulation of
| > general laws of nature" and your "derivation of the laws of physics"?
| >
| > I could try to explain to you but you are too
| > stoooooooooooooooooooooooooopid to learn it. Start by wondering what
| > "derivation" of a law of physics means.
| >
|
| Please explain the difference.
| Here's the difference, we don't know what the laws of nature are, or we
| wouldn't still be trying to find them. I said corretly "laws of
| physics". I apologize for making the necessary correction. Seems a
| pebble is a stumbling block for some.
|
|
| > >
| > > Adios moron. You've stepped in your own ***** once again. One would
| > > think you'd learn something after smelling the stink that follows you
| > > around.
| > >
| >
| > I do not read popular science books like you do, in which physicists
| > try to explain in layma's terms their theories.
|
| Since it's his theory, I supose he should know better than you what to
| call his premises.
|
| >
| > Mike
|
| What's your problem anyway? Do you think that Einstein himself didn't
| make a few statements about existing theory of the negative sort? If
| you'll read his "Ideas and Opinions", you might even wonder why some
| government didn't have him removed. No kidding. He spoke his mind and
| let the chips fall. He was just the sort of guy that I am in that
| sense. I'm only sorry that you have little understanding of the process
| called changing of the guards. It's never a tea party. If you don't
| agree with a statement that's one thing. If your only intent is to
| ***** like a worn out old *****, then you can just gfys.
|
| Richard Perry
I see we have a meeting of the minds, Richard, at least in principle.
I have a strong feeling Mike was shooting from the hip and hit
his own foot.
Mike, take a more careful aim before pulling the trigger, there is
plenty of wild game to shoot at including knuckle-dragging
Neanderthals, Tusselader, pee puppies, phuckwit ducks,
Aunt Sallies, Strawmen, Generals Failure, Generals Moron,
Ghosts, silly geese and various rats and mice. There is even
a snarling catfish called Uncle Al but he's run away complaining
he was in a river of ***** and is now stranded on the river
bank gasping after I hooked him.
Richard is homo sapiens sapiens, if you wish to have a
conversation with him I suggest reason, not conflict. Or you can
return to small game hunting. Remember the old maxim, ticks
and tones may break my bones, but whips and chains excite me.
Androcles
.








User: "Edward Green"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 10:07:27 AM
Sue... wrote:

http://www.bartleby.com/173/23.html

It is not an easy read but seem to suggest the light path from
the rim to hub is affected by

"an effect of inertia (centrifugal force)"

Right or wrong, it seems consistant with Schwarchild's
solution with ~falling light particles~ .

If two wrongs make a right I suppose the answer is

<< 4. The rest of the scientific world: Who cares.>>

You can put it in the same circular file with the
train and embankment story to keep it company
and then go check some maths.

This is a very rare case where I feel obliged to put on my full crank
hat, complete with tassels and plume. I understand the answer, it may
have been published, but, if the material on John Baez's site and
Wikipedia is any gauge of current understanding, it must not be widely
known or appreciated.
Well... that wasn't so cranky... the cranky part is the language I feel
bubbling to the fore without any conscious volition... must fight
it.... something about mathematics losing touch with physics...
mathematical ability seems to be more widely distributed than some
other kind of ability needed here.
There was some talk here some years back about a newly published paper
which I thought had put the thing to rest -- must search for reference.
I don't understand physics at all ... I know most physics papers I look
at seem to be completely beyond my feeble understanding. Yet, when
confronted with the right sort of "paradox", all this machinery beyond
my understanding seems to come up short, while eventually I am able to
work out an answer. Crank words, I know: but I may be right.
.
User: "Sorcerer"

Title: Re: THE EHRENFEST PARADOX 24 Sep 2006 10:46:03 AM
"Edward Green" <spamspamspam3@netzero.com> wrote in message
news:1159110447.727079.305730@i3g2000cwc.googlegroups.com...
| I don't understand physics at all ... I know most physics papers I look
| at seem to be completely beyond my feeble understanding. Yet, when
| confronted with the right sort of "paradox", all this machinery beyond
| my understanding seems to come up short, while eventually I am able to
| work out an answer. Crank words, I know: but I may be right.
Yep... and you may be wrong.
.




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