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Aug 4, 1999, 3:00:00 AM8/4/99

to

Let's consider an interferometer's arm of length L, that makes

an angle a with the velocity vector.

an angle a with the velocity vector.

According to SR, the arm will contract by

f=sqrt(1-v^2) when a=0°, and by f=1 when a=90°.

Iow, L'=L*sqrt(1-v^2) when a=0° and L'=L when a=90°.

Hence, for any angle a other than 0° or 90°, the contraction factor f

must be situated between sqrt(1-v^2) and 1.

Is the general formula giving f,

1) f = sqrt(1-v^2) * cos(a),

2) f = sqrt(1-(v*cos(a))^2), or

3) another formula?

Marcel Luttgens

Aug 4, 1999, 3:00:00 AM8/4/99

to

MLuttgens <mlut...@aol.com> wrote in message

news:19990804055504...@ngol08.aol.com...

> Marcel Luttgens

--

Regards, Cees Roos

I think it's much more interesting to live not knowing than

to have answers which might be wrong. R. Feynman 1981

Aug 5, 1999, 3:00:00 AM8/5/99

to

In article <7o9s7n$e9k$1...@news1.xs4all.nl>, "Cees Roos" <cr...@xs4all.nl> wrote

:

:

>Date : Wed, 4 Aug 1999 18:40:20 +0200

>

>

>MLuttgens <mlut...@aol.com> wrote in message

>news:19990804055504...@ngol08.aol.com...

>> Let's consider an interferometer's arm of length L, that makes

>> an angle a with the velocity vector.

>>

>> According to SR, the arm will contract by

>> f=sqrt(1-v^2) when a=0°, and by f=1 when a=90°.

>> Iow, L'=L*sqrt(1-v^2) when a=0° and L'=L when a=90°.

>> Hence, for any angle a other than 0° or 90°, the contraction factor f

>> must be situated between sqrt(1-v^2) and 1.

>>

>> Is the general formula giving f,

>>

>> 1) f = sqrt(1-v^2) * cos(a),

>> 2) f = sqrt(1-(v*cos(a))^2), or

>> 3) another formula?

>>

>

>f = sqrt((1-v^2)/(1-(v*sin(a))^2))

>

Thank you,

In "Re: To Dennis, Keto and all the Etherists", on Jul 20, 1999,

I already claimed that f=sqrt(1-v^2)/sqrt(1-(v*sin(a))^2) is

the simplest factor that allows to transform T(a) =

(2L/(1-v^2))*sqrt(1-(v*sin(a))^2) to T(a)' = 2L/sqrt(1-v^2),

which is independent of all angles a.

But perhaps did you find in the meantime a direct demonstration

of that factor? It would be much better than reverse

engineering!

Anyhow, there are now 2 formulae matching SR's prediction for

a=0° or a=90°:

1) f = sqrt(1-(v*cos(a))^2)

2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

Which one would Wayne Throop, Tom Roberts, Steve Carlip,

and other SR experts chose? Or another formula?

>Cees Roos

Marcel Luttgens

Aug 5, 1999, 3:00:00 AM8/5/99

to

news:19990805050822...@ngol08.aol.com...[snip]

> >f = sqrt((1-v^2)/(1-(v*sin(a))^2))

> >

>

> Thank you,

>

> In "Re: To Dennis, Keto and all the Etherists", on Jul 20, 1999,

> I already claimed that f=sqrt(1-v^2)/sqrt(1-(v*sin(a))^2) is

> the simplest factor that allows to transform T(a) =

> (2L/(1-v^2))*sqrt(1-(v*sin(a))^2) to T(a)' = 2L/sqrt(1-v^2),

> which is independent of all angles a.

>

> But perhaps did you find in the meantime a direct demonstration

> of that factor? It would be much better than reverse

> engineering!

>

Consider two diagrams:

1: Barlength l' (contracted length), angle a.

> >f = sqrt((1-v^2)/(1-(v*sin(a))^2))

> >

>

> Thank you,

>

> In "Re: To Dennis, Keto and all the Etherists", on Jul 20, 1999,

> I already claimed that f=sqrt(1-v^2)/sqrt(1-(v*sin(a))^2) is

> the simplest factor that allows to transform T(a) =

> (2L/(1-v^2))*sqrt(1-(v*sin(a))^2) to T(a)' = 2L/sqrt(1-v^2),

> which is independent of all angles a.

>

> But perhaps did you find in the meantime a direct demonstration

> of that factor? It would be much better than reverse

> engineering!

>

1: Barlength l' (contracted length), angle a.

/|

/ |

/ |

/ |

l' / | l' * sin(a)

/ |

/ |

/ |

/_a________|

l' * cos(a)

2: Barlength l (uncontracted length), angle a'.

/|

/ |

/ |

/ |

l / | l * sin(a') ( == l' * sin(a) )

/ |

/ |

/ |

/_a'_______|

l * cos(a')

Contraction in x-direction only, so y-sizes equal.

(Excuse me for the diagrams, I'm a lousy ASCII artist)

l'^2 = ( l' * cos(a) )^2 + (l' * sin(a) )^2 =

l'^2 = ( l * cos(a') / gamma(v)) ^2 + (l * sin(a') )^2

= l^2 - ( v * l * cos(a') )^2 (1)

( l * cos(a') )^2 = l^2 * ( 1 - (sin(a') )^2 ) =

= l^2 - ( l * sin(a') )^2

= l^2 - ( l' * sin(a) )^2 (2)

Substitute (2) in (1):

l'^2 = l^2 - v^2 * ( l^2 - ( l' * sin(a) )^2 )

= l^2 - ( v * l )^2 + (v * l' * sin(a) )^2

l'^2 * ( 1 - ( v * sin(a) )^2 ) = l^2 * ( 1 - v^2 )

l'^2 = l^2 * ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 )

l' = l * sqrt( ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 ) )

> Anyhow, there are now 2 formulae matching SR's prediction for

> a=0° or a=90°:

>

Three.

> 1) f = sqrt(1-(v*cos(a))^2)

> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

>

> Which one would Wayne Throop, Tom Roberts, Steve Carlip,

> and other SR experts chose? Or another formula?

>

Aug 5, 1999, 3:00:00 AM8/5/99

to

MLuttgens a écrit dans le message

<19990804055504...@ngol08.aol.com>...

>Let's consider an interferometer's arm of length L, that makes

>an angle a with the velocity vector.

>

>According to SR, the arm will contract by

>f=sqrt(1-v^2) when a=0°, and by f=1 when a=90°.

>Iow, L'=L*sqrt(1-v^2) when a=0° and L'=L when a=90°.

>Hence, for any angle a other than 0° or 90°, the contraction factor f

>must be situated between sqrt(1-v^2) and 1.

>

>Is the general formula giving f,

>

>1) f = sqrt(1-v^2) * cos(a),

>2) f = sqrt(1-(v*cos(a))^2), or

>3) another formula?

It is an other formula.

see http://www.ping.be/electron/mmx.htm

DE WITTE Roland

http://www.ping.be/electron

Under construction.

>

>Marcel Luttgens

Aug 6, 1999, 3:00:00 AM8/6/99

to

In article <7ocges$r55$1...@news1.xs4all.nl>, "Cees Roos" <cr...@xs4all.nl> wrote

:

:

>Date : Thu, 5 Aug 1999 19:08:18 +0200

Your diagrams and demonstration are OK!

>

>l'^2 = ( l' * cos(a) )^2 + (l' * sin(a) )^2 =

>l'^2 = ( l * cos(a') / gamma(v)) ^2 + (l * sin(a') )^2

> = l^2 - ( v * l * cos(a') )^2 (1)

>

>( l * cos(a') )^2 = l^2 * ( 1 - (sin(a') )^2 ) =

> = l^2 - ( l * sin(a') )^2

> = l^2 - ( l' * sin(a) )^2 (2)

>

>Substitute (2) in (1):

>l'^2 = l^2 - v^2 * ( l^2 - ( l' * sin(a) )^2 )

> = l^2 - ( v * l )^2 + (v * l' * sin(a) )^2

>

>l'^2 * ( 1 - ( v * sin(a) )^2 ) = l^2 * ( 1 - v^2 )

>

>l'^2 = l^2 * ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 )

>

>l' = l * sqrt( ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 ) )

>

>

>

>> Anyhow, there are now 2 formulae matching SR's prediction for

>> a=0° or a=90°:

>>

>Three.

>

Which is the third one?

>> 1) f = sqrt(1-(v*cos(a))^2)

>> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

>>

>> Which one would Wayne Throop, Tom Roberts, Steve Carlip,

>> and other SR experts chose? Or another formula?

>>

>> Marcel Luttgens

>--

>Regards, Cees Roos

I will not comment now on your derivation, because I don't

want to influence the other SR experts.

In view of the theoretical significance of such formula, their

opinion is really needed and welcome.

Marcel Luttgens

Aug 6, 1999, 3:00:00 AM8/6/99

to

In article <7oct83$hvr$1...@news.planetinternet.be>, "DE WITTE Roland"

<roland....@ping.be> wrote :

<roland....@ping.be> wrote :

>Date : Thu, 5 Aug 1999 17:40:02 +0100

>

>

>MLuttgens a écrit dans le message

><19990804055504...@ngol08.aol.com>...

>

>>Let's consider an interferometer's arm of length L, that makes

>>an angle a with the velocity vector.

>>

>>According to SR, the arm will contract by

>>f=sqrt(1-v^2) when a=0°, and by f=1 when a=90°.

>>Iow, L'=L*sqrt(1-v^2) when a=0° and L'=L when a=90°.

>>Hence, for any angle a other than 0° or 90°, the contraction factor f

>>must be situated between sqrt(1-v^2) and 1.

>>

>>Is the general formula giving f,

>>

>>1) f = sqrt(1-v^2) * cos(a),

>>2) f = sqrt(1-(v*cos(a))^2), or

>>3) another formula?

>

>It is an other formula.

>see http://www.ping.be/electron/mmx.htm

>

Thank you, I downloaded you page, but it would be better

to present your derivation in the NG.

Anyhow, I don't see any difference between your formula

and that of Cees Roos.

Aug 6, 1999, 3:00:00 AM8/6/99

to

news:19990806050850...@ngol02.aol.com...[snip]

> >l' = l * sqrt( ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 ) )

> >

> >

> >

> >> Anyhow, there are now 2 formulae matching SR's prediction for

> >> a=0° or a=90°:

> >>

> >Three.

> >

>

> Which is the third one?

>

The one I gave you !-)

> >l' = l * sqrt( ( 1 - v^2 ) / ( 1 - ( v * sin(a) )^2 ) )

> >

> >

> >

> >> Anyhow, there are now 2 formulae matching SR's prediction for

> >> a=0° or a=90°:

> >>

> >Three.

> >

>

> Which is the third one?

>

> >> 1) f = sqrt(1-(v*cos(a))^2)

> >> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

> >>

> >> Which one would Wayne Throop, Tom Roberts, Steve Carlip,

> >> and other SR experts chose? Or another formula?

> >>

> >> Marcel Luttgens

> >--

> >Regards, Cees Roos

>

> I will not comment now on your derivation, because I don't

> want to influence the other SR experts.

> In view of the theoretical significance of such formula, their

> opinion is really needed and welcome.

>

> Marcel Luttgens

--

Regards, Cees Roos

Aug 6, 1999, 3:00:00 AM8/6/99

to

MLuttgens a écrit dans le message

>>>Is the general formula giving f,

>>>

>>>1) f = sqrt(1-v^2) * cos(a),

>>>2) f = sqrt(1-(v*cos(a))^2), or

>>>3) another formula?

>>

>>It is an other formula.

>>see http://www.ping.be/electron/mmx.htm

>>

>

>Thank you, I downloaded you page, but it would be better

>to present your derivation in the NG.

It is difficult without geometric figures. I think that at present everybody

has Internet explorer 4 with the possibility to clic on the web-site page

address.

>Anyhow, I don't see any difference between your formula

>and that of Cees Roos.

Yes, may be, I don't read all the messages, but often only the headers of

the threads. That because my ideas are nearly always different than the

other peoples in this newsgroup.

Aug 9, 1999, 3:00:00 AM8/9/99

to

: mlut...@aol.com (MLuttgens)

: Anyhow, there are now 2 formulae matching SR's prediction for

: a=0° or a=90°:

: 1) f = sqrt(1-(v*cos(a))^2)

: 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

:

: Which one would Wayne Throop, Tom Roberts, Steve Carlip,

: and other SR experts chose? Or another formula?

: Anyhow, there are now 2 formulae matching SR's prediction for

: a=0° or a=90°:

: 1) f = sqrt(1-(v*cos(a))^2)

: 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

:

: Which one would Wayne Throop, Tom Roberts, Steve Carlip,

: and other SR experts chose? Or another formula?

MLuttgens is going around pretending there's some difficulty with the

correct expression of the length of a moving rod when oriented at an

angle to motion. Note: MLuttgens has actually also pretended that

deriving this distance in terms of a rod was invalid, since in an

interferometer, there neen not be a literal rod. But the discussion is

about two endpoints and a distance between them. Whether that distance

is occupied by a rod is completely irrelevant; I state the problem in

terms of "a rod" simply for illustrative purposes. MLuttgens'

"there might not be a rod" objection is ludicrous.

In SR or LET, the x-extent of the rod is foreshortened in the

coordinate system in which the rod moves, so there is no difficulty at all.

The length is

L' = L*sqrt(cos(a)^2*(1-v^2)+sin(a)^2)

= sqrt(cos(a)^2+sin(a)^2-v^2cos(a)^2))

= sqrt(1-(v*cos(a))^2)

To say this "matches SR's prediction for 0 or 90 degrees"

is a ridiculous understatement. That is SR's predicted arm length

for any angle "a".

Note: the angle "a" is the angle in the comoving coordinate system (or

in LET, measured with a comoving protractor). If you want it as a

function of an angle "b" in the non-comoving coordinate system (or in

LET, measured with a protractor "at rest"), you substitute

a=atan(tan(b)/sqrt(1-v^2)).

Now, since we find that for all angles "a" (measured in the comoving

frame), the light bounce time along that arm (in the non-comoving frame)

is 2*L/sqrt(1-v^2). So, if we want the form in terms of "b", so

everything is from the viewpoint of the non-comoving frame, we just

substitute for all atan(tan(b)/sqrt(1-v^2)) for all "a"s in that

formula. Go ahead, MLuttgens; do that. Be sure to replace

every single "a" in 2*L/sqrt(1-v^2). What do you get?

Now... what controversy or puzzle is supposed to be lurking here?

The whole thing is simple, straightforward, and unambiguous.

MLuttgens himself did the derivation of 2*L/sqrt(1-v^2) given "a".

It's a bit tricky as such things go, but not really all that

difficult; nothing past high-school trig.

So why does he pretend there's a problem here? I dunno.

I first thought, it's idiocy. Then I thought, it's an intentional

lie, and hence malice. Now I don't know. There's just no explaining

MLuttgens' behavior logically at all.

Wayne Throop thr...@sheol.org http://sheol.org/throopw

Aug 9, 1999, 3:00:00 AM8/9/99

to

In article <9341...@sheol.org>, thr...@sheol.org (Wayne Throop) wrote :

>Date : Mon, 09 Aug 1999 00:03:29 GMT

>

>: mlut...@aol.com (MLuttgens)

>: Anyhow, there are now 2 formulae matching SR's prediction for

>: a=0° or a=90°:

>: 1) f = sqrt(1-(v*cos(a))^2)

>: 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

>:

>: Which one would Wayne Throop, Tom Roberts, Steve Carlip,

>: and other SR experts chose? Or another formula?

>

>MLuttgens is going around pretending there's some difficulty with the

>correct expression of the length of a moving rod when oriented at an

>angle to motion. Note: MLuttgens has actually also pretended that

>deriving this distance in terms of a rod was invalid, since in an

>interferometer, there neen not be a literal rod. But the discussion is

>about two endpoints and a distance between them. Whether that distance

>is occupied by a rod is completely irrelevant; I state the problem in

>terms of "a rod" simply for illustrative purposes. MLuttgens'

>"there might not be a rod" objection is ludicrous.

>

>In SR or LET, the x-extent of the rod is foreshortened in the

>coordinate system in which the rod moves, so there is no

>difficulty at all.

So you keep claiming that the contracted projection of the

arm has a physical meaning, and can be used to calculate

the contracted length of a moving rod when oriented at an

angle to motion.

Imagine now that the arm is situated on the x-axis,

and the velocity vector makes an angle a with the x-axis?

What would be your derivation of the contraction factor f

in such case?

Thank you. About the "Now, I don't know", which is true,

just wait and see.

To recap, the relevant formulae are

1) f = sqrt(1-(v*cos(a))^2)

According to WayneThroop (see above),

"L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

arm length for any angle "a", "a" being the angle

measured in the comoving coordinate system.

2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

(Cees Roos and De Witte)

The "whole thing" is far from being "simple, straightforward, and unambiguous".

What is the opinion of Tom Roberts, Steve Carlip and

other SR experts?

Marcel Luttgens

Aug 9, 1999, 3:00:00 AM8/9/99

to

: mlut...@aol.com (MLuttgens)

: So you keep claiming that the contracted projection of the arm has a

: physical meaning, and can be used to calculate the contracted length

: of a moving rod when oriented at an angle to motion.

: So you keep claiming that the contracted projection of the arm has a

: physical meaning, and can be used to calculate the contracted length

: of a moving rod when oriented at an angle to motion.

Liar. You know very well that that's not what I said,

nor is it implied by anything I've said. I can't "keep claiming"

things you mistake me for saying or implying.

The arms directional contraction has a physical meaning. The projection

onto a coordinate axis is conventional. And MLuttgens knew that,

because he'd brought up the exact same bogus objection before.

: The "whole thing" is far from being "simple, straightforward, and

: unambiguous".

Only in what passes for MLuttgens' "mind".

Aug 10, 1999, 3:00:00 AM8/10/99

to

: mlut...@aol.com (MLuttgens)

: 1) f = sqrt(1-(v*cos(a))^2)

: According to WayneThroop (see above),

: "L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

: arm length for any angle "a", "a" being the angle

: measured in the comoving coordinate system.

:

: 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

: (Cees Roos and De Witte)

: 1) f = sqrt(1-(v*cos(a))^2)

: According to WayneThroop (see above),

: "L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

: arm length for any angle "a", "a" being the angle

: measured in the comoving coordinate system.

:

: 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

: (Cees Roos and De Witte)

By the way, what makes you think those are two distinct cases?

Hint: in (1), the angle is measured in the comoving frame.

but in (2), the angle is measured in the non-comoving frame.

An issue which has been explained to MLuttgens several times,

to no noticeable effect.

: The "whole thing" is far from being "simple, straightforward,

: and unambiguous".

Sorry. Still simple. Still straightforward. Still unambiguous.

Aug 10, 1999, 3:00:00 AM8/10/99

to

NB:

WT = Wayne Throop, ML = MLuttgens

WT = Wayne Throop, ML = MLuttgens

WT:

In SR or LET, the x-extent of the rod is foreshortened in the

coordinate system in which the rod moves, so there is no

difficulty at all.

ML:

So you keep claiming that the contracted projection of the

arm has a physical meaning, and can be used to calculate

the contracted length of a moving rod when oriented at an

angle to motion.

WT:

Liar. You know very well that that's not what I said,

nor is it implied by anything I've said. I can't "keep claiming"

things you mistake me for saying or implying.

The arms directional contraction has a physical meaning.

The projection onto a coordinate axis is conventional.

And MLuttgens knew that, because he'd brought up the exact

same bogus objection before.

ML(new):

It is perhaps not what you said, but it is implied by your

derivation.

Btw, does "conventional" means: "depending on or conforming

to formal or accepted standards or rules rather than nature"?

Could you elaborate a little further?

ML:

Imagine now that the arm is situated on the x-axis,

and the velocity vector makes an angle a with the x-axis?

What would be your derivation of the contraction factor f

in such case?

ML(new):

No reaction from WT to that scenario.

Does it mean that WT is unable to derive f in that case?

ML:

To recap, the relevant formulae are

1) f = sqrt(1-(v*cos(a))^2)

According to WayneThroop (see above),

"L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

arm length for any angle "a", "a" being the angle

measured in the comoving coordinate system.

2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

(Cees Roos and De Witte)

WT:

By the way, what makes you think those are two distinct cases?

Hint: in (1), the angle is measured in the comoving frame.

but in (2), the angle is measured in the non-comoving frame.

ML(new):

The angles in the two formulae are related according to

the relation sin(a') = sin(a) / sqrt(1-(v^cos(a))^2), hence (2)

should read f = sqrt((1-v^2)/(1-(v*sin(a'))^2)).

Marcel Luttgens

Aug 10, 1999, 3:00:00 AM8/10/99

to

::: mlut...@aol.com (MLuttgens)

::: So you keep claiming that the contracted projection of the arm has a

::: physical meaning, and can be used to calculate the contracted length

::: of a moving rod when oriented at an angle to motion.

::: So you keep claiming that the contracted projection of the arm has a

::: physical meaning, and can be used to calculate the contracted length

::: of a moving rod when oriented at an angle to motion.

:: thr...@sheol.org (Wayne Throop)

:: You know very well that that's not what I said, nor is it implied by

:: anything I've said. I can't "keep claiming" things you mistake me

:: for saying or imply

: mlut...@aol.com (MLuttgens)

: It is perhaps not what you said, but it is implied by your derivation.

Why MLuttgens bothers lying about things like this is beyond me.

A projection is not physical, I never said it was, and I never said

anything that implies that it is.

The derivation uses coordinates; in particular, distance measures

from a standard origin. Coordinates are not themselves physical.

Therefore, the simple use of length contraction on standard

coordinates has no implication whatsoever that a projection is physical.

So what *is* physical? The contraction of physical objects in the

direction of motion. If you lay out coordinates using such physical objects,

you get a coordinate system foreshortened in the direction of travel.

And this has all been explained to MLuttgens several times already.

:: By the way, what makes you think those are two distinct cases? Hint:

:: in (1), the angle is measured in the comoving frame. but in (2), the

:: angle is measured in the non-comoving frame.

: The angles in the two formulae are related according to the relation

: sin(a') = sin(a) / sqrt(1-(v^cos(a))^2), hence (2) should read f =

: sqrt((1-v^2)/(1-(v*sin(a'))^2)).

So, you expect people to use a terminology you've just newly invented ?

And why is (a') the angle in "stationary" coordinates, while (a) is the

angle in "moving" coordinates, opposite of the usual conventions?

I explicitly said what I meant by "a"; you have no excuse to now pretend

I was being unclear in any way whatsoever, or that my terminology is

suddenly "wrong", when you knew exactly what I meant all along.

Slimy weasel.

The fact remains: the two forms are identical, once you realize (as is

obvious) that one is expressed as a function of the angle in comoving

coordinates, and the other ie expressed as a function of the angle in

non-comoving coordinates. No ammount of MLuttgens' squirming and

wriggling and thrashing about will change this simple fact.

Aug 12, 1999, 3:00:00 AM8/12/99

to

MLuttgens wrote:

> Anyhow, there are now 2 formulae matching SR's prediction for

> a=0° or a=90°:

> 1) f = sqrt(1-(v*cos(a))^2)

> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

> Anyhow, there are now 2 formulae matching SR's prediction for

> a=0° or a=90°:

> 1) f = sqrt(1-(v*cos(a))^2)

> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

In SR it is impossible to come up with a truly meaningful formula for

this -- this is not a purely spatial situation in SR when viewed from

another frame.

Other posters have provided the SR formula for this, as asked.

But I think the entire question and underlying approach are

flawed.

SR is more than length contraction, and you are attempting to consider

just the length contraction of a rod (or distance between two points

at rest in the frame). When viewed from another frame there is an

admixture of time difference between the points, as well as a different

spatial difference. Your entire approach ignores this basic fact.

That is (viewing from another frame), as a varies not only

does the spatial distance between the endpoints vary but also

the time difference varies (for events at the endpoints of the

rod which are simultaneous in the rest frame of the rod).

Attempting to ignore this variation in time difference

frequently/usually leads you to wrong conclusions.

In general it is invalid to "take a shortcut" and just consider

length contraction; you must use the full Lorentz transform, and

you must consider specific events, not merely endpoints of a rod --

the latter includes too much ambiguity in other frames. Ditto for

time dilation.

This _does_ depends upon how you use the result. In some specific

cases it may be valid to use the results given by other posters.

But in general it is easy to get into trouble with shortcuts like

this....

If, say, you want to analyze the MMX in SR, then the best

approach is to use the invariance of c, and avoid any

transforms at all! Such invariance principles are _MUCH_

more powerful than slogging through the details of the

coordinate transforms. Note that length contraction alone

cannot give that invariance, nor can length contraction

plus time dilation; it takes the full Lorentz transform

to demonstrate the invariance of c.

Exercise: compare and contrast the use of invariance

principles like this vs coordinate transforms to the use

of energy conservation vs F=ma in Newtonian mechanics.

Advanced exercise: compare and contrast to Lagrangian vs

Newtonian mechanics, and Hamiltonian vs Newtonian mechanics.

Tom Roberts tjro...@lucent.com

Aug 13, 1999, 3:00:00 AM8/13/99

to

In article <37B2DEFF...@lucent.com>, Tom Roberts <tjro...@lucent.com>

wrote :

wrote :

>of a rod --the latter includes too much ambiguity in other

>frames. Ditto for time dilation.

>

>This _does_ depends upon how you use the result.

>In some specific cases it may be valid to use the results

>given by other posters.

>But in general it is easy to get into trouble with shortcuts like

>this....

>

> If, say, you want to analyze the MMX in SR, then the best

> approach is to use the invariance of c, and avoid any

> transforms at all! Such invariance principles are _MUCH_

> more powerful than slogging through the details of the

> coordinate transforms. Note that length contraction alone

> cannot give that invariance, nor can length contraction

> plus time dilation; it takes the full Lorentz transform

> to demonstrate the invariance of c.

>

> Exercise: compare and contrast the use of invariance

> principles like this vs coordinate transforms to the use

> of energy conservation vs F=ma in Newtonian mechanics.

> Advanced exercise: compare and contrast to Lagrangian vs

> Newtonian mechanics, and Hamiltonian vs Newtonian

> mechanics.

>

>

>Tom Roberts

Thank you for this interesting analysis of the problem.

I cannot pretend that I am surprised at the impossibility, in SR,

to come up with a truly meaningful formula, essentially, Imo,

because the derivation of the Lorentz transform was based

on two frames of reference in uniform relative translatory

motion and the consideration of light signals sent along

the x' and y'-axes, and certainly not of signals making some

angle with the coordinate axes.

So, I am inclined to thinking that the Lorentz transform itself

is moot, and that a more general transform, not limited to

angles of 0° and 90°, should be derived. In any case, such

an approach can only be fruitful, much more than going round

in circles for months.

The new transform would probably show that the

interferometer's arms contract according to sqrt(1-(v*cos(a))^2),

and that the angle a between arm and velocity vector

is frame independent. Let's note that a is measured in the

interferometer frame.

Otoh, in the second formula f = sqrt((1-v^2)/(1-(v*sin(a))^2)),

a is measured in the non-comoving frame (the frame at rest

in the ether). Using the present Lorentz transform, and

calling b that new angle a, one finds that cos(a)^2 =

(1-(sin(b))^2)/(1-(v*sin(b))^2). Replacing cos(a)^2 by that

value in f=sqrt(1-(v*cos(a))^2), the second formula is readily

obtained. But if a is frame independent, the second formula

is of course false.

As an approach to derive a general Lorentz transform,

one could first consider an arm of length L making an angle

of 45° with the velocity vector v situated on the x_axis. By

following the same steps as Lorentz in his demonstration,

one would obtain

gamma=1/sqrt(1-(v*cos(45))^2)

x'=gamma(x-v*cos(45)*t) y'=y

t'=gamma(t-v*cos(45)*x)

But one could as well imagine that the velocity vector is situated

on the y-axis, and obtain a perfect symmetrical result:

gamma=1/sqrt(1-(v*sin(45))^2)

y'=gamma(y-v*sin(45)*t) x'=x

t'=gamma(t-v*sin(45)*y)

Hence, in vue of that symmetry, it is impossible for the angle a

to change, because its anti-clockwise increase (velocity vector

along x) is exactly compensated by its clockwise decrease

(vector along y).

Marcel Luttgens

Aug 13, 1999, 3:00:00 AM8/13/99

to MLuttgens

MLuttgens wrote:

>

> To recap, the relevant formulae are

>

> 1) f = sqrt(1-(v*cos(a))^2)

> According to WayneThroop (see above),

> "L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

> arm length for any angle "a", "a" being the angle

> measured in the comoving coordinate system.

>

> To recap, the relevant formulae are

>

> 1) f = sqrt(1-(v*cos(a))^2)

> According to WayneThroop (see above),

> "L'=L*sqrt(1-(v*cos(a))^2), which is SR's predicted

> arm length for any angle "a", "a" being the angle

> measured in the comoving coordinate system.

Correct.

> 2) f = sqrt((1-v^2)/(1-(v*sin(a))^2))

> (Cees Roos and De Witte)

Which is also correct, but the angle a in this equation

is the angle of the _moving_ rod in the "ether frame",

e.g. in the frame where the rod is moving with the speed v.

If we rename this angle to a', we will have the following

relationship between these angles:

sin(a') = sin(a)/sqrt(1-(v*cos(a))^2)

a = angle in the rod frame

a'= angle in the "ether frame"

if you insert this in 2) you will get 1) above.

> The "whole thing" is far from being "simple, straightforward,

> and unambiguous".

What exactly do you find so difficult about this?

However, this length is not very significant regarding the MMX.

In the frame where the rod is moving, the important question

is the length the light have to go forth and back the rod,

and as the rod is moving, it should be quite obvious that

this length is not twice the length of the rod.

In fact, it is according to SR: LP = 2*L/sqrt(1-v^2)

(I am to lazy to show the calculations right now,

but I probably will if provoked. :-) )

Since it is independent of the angle of the rod, SR predicts

a null result for the MMX for any angle between the two rods,

not only pi/2.

Paul

Aug 13, 1999, 3:00:00 AM8/13/99

to

Utter nonsense. :-)

Of course it does not matter in which direction the light

or anything else moves.

> So, I am inclined to thinking that the Lorentz transform itself

> is moot, and that a more general transform, not limited to

> angles of 0° and 90°, should be derived. In any case, such

> an approach can only be fruitful, much more than going round

> in circles for months.

You are right about the circles.

You see problems where none are.

From where have you got the strange idea that there

is a problem with the LT if the light goes in other

directions than along the axes?

> The new transform would probably show that the

> interferometer's arms contract according to sqrt(1-(v*cos(a))^2),

> and that the angle a between arm and velocity vector

> is frame independent. Let's note that a is measured in the

> interferometer frame.

But why would you want this angle to be frame independent?

> Otoh, in the second formula f = sqrt((1-v^2)/(1-(v*sin(a))^2)),

> a is measured in the non-comoving frame (the frame at rest

> in the ether).

Right.

> Using the present Lorentz transform, and

> calling b that new angle a, one finds that cos(a)^2 =

> (1-(sin(b))^2)/(1-(v*sin(b))^2).

Right.

cos(a) = cos(b)/sqrt(1-(v*sin(b))^2)

and

sin(b) = sin(a)/sqrt(1-(v*sin(a))^2)

> Replacing cos(a)^2 by that

> value in f=sqrt(1-(v*cos(a))^2), the second formula is readily

> obtained.

Right.

> But if a is frame independent, the second formula

> is of course false.

But the angle is frame dependent and the second

formula is right as is the first.

So what's the problem?

> As an approach to derive a general Lorentz transform,

> one could first consider an arm of length L making an angle

> of 45° with the velocity vector v situated on the x_axis. By

> following the same steps as Lorentz in his demonstration,

> one would obtain

> gamma=1/sqrt(1-(v*cos(45))^2)

> x'=gamma(x-v*cos(45)*t) y'=y

> t'=gamma(t-v*cos(45)*x)

> But one could as well imagine that the velocity vector is situated

> on the y-axis, and obtain a perfect symmetrical result:

> gamma=1/sqrt(1-(v*sin(45))^2)

> y'=gamma(y-v*sin(45)*t) x'=x

> t'=gamma(t-v*sin(45)*y)

> Hence, in vue of that symmetry, it is impossible for the angle a

> to change, because its anti-clockwise increase (velocity vector

> along x) is exactly compensated by its clockwise decrease

> (vector along y).

>

> Marcel Luttgens

Tell me, which problem are you seeing with the Lorentz transform

since you think a new should be derived?

You have got your answers:

L' = L*sqrt(1-(v*cos(a))^2) - a angle in rod frame

L' = L*sqrt((1-v^2)/(1-(v*sin(a))^2)) - a angle in "ether frame"

The answers are identical. So what's the problem?

Is it that you have not realized that the rod length

ìn the ether frame is not very significant for the MMX?

Paul

Aug 14, 1999, 3:00:00 AM8/14/99

to

In article <37B4635F...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

It does matter for the MMX analysis.

>> So, I am inclined to thinking that the Lorentz transform itself

>> is moot, and that a more general transform, not limited to

>> angles of 0° and 90°, should be derived. In any case, such

>> an approach can only be fruitful, much more than going round

>> in circles for months.

>

>You are right about the circles.

>You see problems where none are.

>From where have you got the strange idea that there

>is a problem with the LT if the light goes in other

>directions than along the axes?

>

Why don't you try to derive the general LT first?

>> The new transform would probably show that the

>> interferometer's arms contract according to sqrt(1-(v*cos(a))^2),

>> and that the angle a between arm and velocity vector

>> is frame independent. Let's note that a is measured in the

>> interferometer frame.

>

>But why would you want this angle to be frame independent?

>

It is fundamental for the correct interpretation of the MMX.

>> Otoh, in the second formula f = sqrt((1-v^2)/(1-(v*sin(a))^2)),

>> a is measured in the non-comoving frame (the frame at rest

>> in the ether).

>

>Right.

>

>> Using the present Lorentz transform, and

>> calling b that new angle a, one finds that cos(a)^2 =

>> (1-(sin(b))^2)/(1-(v*sin(b))^2).

>

>Right.

> cos(a) = cos(b)/sqrt(1-(v*sin(b))^2)

>and

> sin(b) = sin(a)/sqrt(1-(v*sin(a))^2)

>

>> Replacing cos(a)^2 by that

>> value in f=sqrt(1-(v*cos(a))^2), the second formula is readily

>> obtained.

>

>Right.

>

>> But if a is frame independent, the second formula

>> is of course false.

>

>But the angle is frame dependent and the second

>formula is right as is the first.

>So what's the problem?

>

How would you derive the LT if the arm is on the x-axis,

and the velocity vector made an angle of 45° with the arm?

Would you still find that a is frame dependent?

You are just asserting without really knowing.

>> As an approach to derive a general Lorentz transform,

>> one could first consider an arm of length L making an angle

>> of 45° with the velocity vector v situated on the x_axis. By

>> following the same steps as Lorentz in his demonstration,

>> one would obtain

>> gamma=1/sqrt(1-(v*cos(45))^2)

>> x'=gamma(x-v*cos(45)*t) y'=y

>> t'=gamma(t-v*cos(45)*x)

>> But one could as well imagine that the velocity vector is situated

>> on the y-axis, and obtain a perfect symmetrical result:

>> gamma=1/sqrt(1-(v*sin(45))^2)

>> y'=gamma(y-v*sin(45)*t) x'=x

>> t'=gamma(t-v*sin(45)*y)

>> Hence, in vue of that symmetry, it is impossible for the angle a

>> to change, because its anti-clockwise increase (velocity vector

>> along x) is exactly compensated by its clockwise decrease

>> (vector along y).

>>

>> Marcel Luttgens

>

>Tell me, which problem are you seeing with the Lorentz transform

>since you think a new should be derived?

>

The problem is that the present LT is not general

>You have got your answers:

>L' = L*sqrt(1-(v*cos(a))^2) - a angle in rod frame

>L' = L*sqrt((1-v^2)/(1-(v*sin(a))^2)) - a angle in "ether frame"

>

>The answers are identical. So what's the problem?

>

They are identical only if one assumes length contraction.

Or such contraction has never been experimentally observed.

Without length contraction, the correct formula is the first one,

where f=sqrt(1-(v*cos(a))^2) is a time slowing factor.

>Is it that you have not realized that the rod length

>ìn the ether frame is not very significant for the MMX?

>

>Paul

Lucky are those who blindly believe!

Marcel Luttgens

Aug 15, 1999, 3:00:00 AM8/15/99

to

: "Paul B. Andersen" <paul.b....@hia.no>

: However, this length is not very significant regarding the MMX.

:

: In the frame where the rod is moving, the important question

: is the length the light have to go forth and back the rod,

: and as the rod is moving, it should be quite obvious that

: this length is not twice the length of the rod.

:

: In fact, it is according to SR: LP = 2*L/sqrt(1-v^2)

:

: (I am to lazy to show the calculations right now,

: but I probably will if provoked. :-) )

: However, this length is not very significant regarding the MMX.

:

: In the frame where the rod is moving, the important question

: is the length the light have to go forth and back the rod,

: and as the rod is moving, it should be quite obvious that

: this length is not twice the length of the rod.

:

: In fact, it is according to SR: LP = 2*L/sqrt(1-v^2)

:

: (I am to lazy to show the calculations right now,

: but I probably will if provoked. :-) )

It's been done. With no detectable effect on MLuttgens' strange claims.

No, wait: there *was* one effect: he then claimed that length contraction

changed both x and y displacements between the endpoints; implicitly,

in such a way as to keep the angle a=a' for all orientations. Sigh.

Aug 15, 1999, 3:00:00 AM8/15/99

to

: Tom Roberts

: If, say, you want to analyze the MMX in SR, then the best approach is

: to use the invariance of c, and avoid any transforms at all! Such

: invariance principles are _MUCH_ more powerful than slogging through

: the details of the coordinate transforms. Note that length

: contraction alone cannot give that invariance, nor can length

: contraction plus time dilation; it takes the full Lorentz transform to

: demonstrate the invariance of c.

: If, say, you want to analyze the MMX in SR, then the best approach is

: to use the invariance of c, and avoid any transforms at all! Such

: invariance principles are _MUCH_ more powerful than slogging through

: the details of the coordinate transforms. Note that length

: contraction alone cannot give that invariance, nor can length

: contraction plus time dilation; it takes the full Lorentz transform to

: demonstrate the invariance of c.

Of course; I agree fully. Use of SR's invariants is just a

good-old-fashioned-simpler way of looking at things.

But the point here is not to analyze MM. It's to convince MLuttgens

that the invariants actually work correctly; that it really does not

matter which frame you do the calculation in, you get the same answer.

Therefore, we know, immediately, that there are exactly zero fringe

shifts in the gadget's rest frame. The task is then to show MLuttgens

the tedious-but-basically-simple fact of the matter: you also get zero

frings shifts in ALL OTHER frames as well.

So how did "length contraction alone" get into it? Well, that's because

MLuttgens claims that "time dilation alone" can account for MM (as opposed

to other experiments), which is clearly incorrect. It's a historical

artifact of the discussion path. Neither one gives invariance, but

1: time dilation cannot ex plain MM, and 2: length contraction can.

And finally, MLuttgens has some strange notion of length contraction

which is not LET nor SR length contraction: the angle "a" between a

coordinate axis and a line containing two points is invariant across

a boost in MLuttgens' bizzaro-world version.

Aug 15, 1999, 3:00:00 AM8/15/99

to

:: Of course it does not matter in which direction the light

:: or anything else moves.

:: or anything else moves.

: mlut...@aol.com (MLuttgens)

: It does matter for the MMX analysis.

Wrong, of course; demonstrably so.

The round trip times are equal no matter the direction.

: I cannot pretend that I am surprised at the impossibility, in SR, to

: come up with a truly meaningful formula,

The SR formula is perfectly meaningful.

Just because MLuttgens pretends it has no meaning

is not a flaw in SR's predicted results.

Aug 16, 1999, 3:00:00 AM8/16/99

to

MLuttgens wrote:

>

> In article <37B4635F...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >

> >MLuttgens wrote:

> >>

> >> I cannot pretend that I am surprised at the impossibility, in SR,

> >> to come up with a truly meaningful formula, essentially, Imo,

> >> because the derivation of the Lorentz transform was based

> >> on two frames of reference in uniform relative translatory

> >> motion and the consideration of light signals sent along

> >> the x' and y'-axes, and certainly not of signals making some

> >> angle with the coordinate axes.

> >

> >Utter nonsense. :-)

> >Of course it does not matter in which direction the light

> >or anything else moves.

> >

>

> It does matter for the MMX analysis.

>

> In article <37B4635F...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >

> >MLuttgens wrote:

> >>

> >> I cannot pretend that I am surprised at the impossibility, in SR,

> >> to come up with a truly meaningful formula, essentially, Imo,

> >> because the derivation of the Lorentz transform was based

> >> on two frames of reference in uniform relative translatory

> >> motion and the consideration of light signals sent along

> >> the x' and y'-axes, and certainly not of signals making some

> >> angle with the coordinate axes.

> >

> >Utter nonsense. :-)

> >Of course it does not matter in which direction the light

> >or anything else moves.

> >

>

> It does matter for the MMX analysis.

The point is that the LT obviously can handle light

going in any direction.

> >> So, I am inclined to thinking that the Lorentz transform itself

> >> is moot, and that a more general transform, not limited to

> >> angles of 0° and 90°, should be derived. In any case, such

> >> an approach can only be fruitful, much more than going round

> >> in circles for months.

> >

> >You are right about the circles.

> >You see problems where none are.

> >From where have you got the strange idea that there

> >is a problem with the LT if the light goes in other

> >directions than along the axes?

> >

>

> Why don't you try to derive the general LT first?

What do you mean by that?

Do you mean with the boost in a general direction

not along the x-axis?

Of course you can express the LT with the boost in a general

direction. I don't have to derive it. It's done.

> >> The new transform would probably show that the

> >> interferometer's arms contract according to sqrt(1-(v*cos(a))^2),

> >> and that the angle a between arm and velocity vector

> >> is frame independent. Let's note that a is measured in the

> >> interferometer frame.

> >

> >But why would you want this angle to be frame independent?

> >

>

> It is fundamental for the correct interpretation of the MMX.

Indeed.

The frame dependence of this angle is due to the velocity dependent

shortening of the rod which is necessary to explain the MMX.

> >> Otoh, in the second formula f = sqrt((1-v^2)/(1-(v*sin(a))^2)),

> >> a is measured in the non-comoving frame (the frame at rest

> >> in the ether).

> >

> >Right.

> >

> >> Using the present Lorentz transform, and

> >> calling b that new angle a, one finds that cos(a)^2 =

> >> (1-(sin(b))^2)/(1-(v*sin(b))^2).

> >

> >Right.

> > cos(a) = cos(b)/sqrt(1-(v*sin(b))^2)

> >and

> > sin(b) = sin(a)/sqrt(1-(v*sin(a))^2)

> >

> >> Replacing cos(a)^2 by that

> >> value in f=sqrt(1-(v*cos(a))^2), the second formula is readily

> >> obtained.

> >

> >Right.

> >

> >> But if a is frame independent, the second formula

> >> is of course false.

> >

> >But the angle is frame dependent and the second

> >formula is right as is the first.

> >So what's the problem?

> >

>

> How would you derive the LT if the arm is on the x-axis,

> and the velocity vector made an angle of 45° with the arm?

Use the LT with the boost in that direction, of course.

> Would you still find that a is frame dependent?

Yes, the angle of the rod is frame dependent. Period.

However, the angle will be the same for all frames which

are moving in such a way that the angle between the rod and

the velocity vector happens to be 0 or pi/2.

So what?

> You are just asserting without really knowing.

Asserting what without knowing?

> >> As an approach to derive a general Lorentz transform,

> >> one could first consider an arm of length L making an angle

> >> of 45° with the velocity vector v situated on the x_axis. By

> >> following the same steps as Lorentz in his demonstration,

> >> one would obtain

> >> gamma=1/sqrt(1-(v*cos(45))^2)

> >> x'=gamma(x-v*cos(45)*t) y'=y

> >> t'=gamma(t-v*cos(45)*x)

> >> But one could as well imagine that the velocity vector is situated

> >> on the y-axis, and obtain a perfect symmetrical result:

> >> gamma=1/sqrt(1-(v*sin(45))^2)

> >> y'=gamma(y-v*sin(45)*t) x'=x

> >> t'=gamma(t-v*sin(45)*y)

> >> Hence, in vue of that symmetry, it is impossible for the angle a

> >> to change, because its anti-clockwise increase (velocity vector

> >> along x) is exactly compensated by its clockwise decrease

> >> (vector along y).

> >>

> >> Marcel Luttgens

> >

> >Tell me, which problem are you seeing with the Lorentz transform

> >since you think a new should be derived?

> >

>

> The problem is that the present LT is not general.

If you by "the present LT" mean the expression for the LT written

in it's most common form with the boost in the x-direction,

so no - _that form_ is not general. Obviously.

But the LT as such is.

> >You have got your answers:

> >L' = L*sqrt(1-(v*cos(a))^2) - a angle in rod frame

> >L' = L*sqrt((1-v^2)/(1-(v*sin(a))^2)) - a angle in "ether frame"

> >

> >The answers are identical. So what's the problem?

> >

>

> They are identical only if one assumes length contraction.

> Or such contraction has never been experimentally observed.

But it's consequences are.

> Without length contraction, the correct formula is the first one,

> where f=sqrt(1-(v*cos(a))^2) is a time slowing factor.

Ah. That nonsense again.

There is only in a fantasy world that coinciding events are

not coinciding in every frame of reference.

That is quite impossible in the real world.

> >Is it that you have not realized that the rod length

> >ìn the ether frame is not very significant for the MMX?

> >

> >Paul

>

> Lucky are those who blindly believe!

Indeed.

Blindly believing that the MMX somehow can be explained

by a _direction dependent_ time dilation is -

well - a blind belief.

It would vaporize the moment you open your eyes.

BTW, I cannot understand where you are heading with all

this nonsense about the LT.

You do understand that the LT explains the MMX just fine.

Or don't you?

Paul

Aug 17, 1999, 3:00:00 AM8/17/99

to

In article <37B7BC24...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

MLuttgens:

The angle a between arm and velocity vector, measured in the

interferometer frame, is frame independent.

P.B. Andersen:

The angle of the rod is frame dependent. Period.

However, the angle will be the same for all frames which

are moving in such a way that the angle between the rod and

the velocity vector happens to be 0 or pi/2.

You have got your answers:

L' = L*sqrt(1-(v*cos(a))^2) - a angle in rod frame

L' = L*sqrt((1-v^2)/(1-(v*sin(a))^2)) - a angle in "ether frame"

The answers are identical. So what's the problem?

MLuttgens:

They are identical only if one assumes length contraction.

Or such contraction has never been experimentally observed.

P.B. Andersen:

But it's consequences are.

MLuttgens:

Without length contraction, the correct formula is the first one,

where f=sqrt(1-(v*cos(a))^2) is a time slowing factor.

P.B. Andersen

Ah. That nonsense again.

There is only in a fantasy world that coinciding events are

not coinciding in every frame of reference.

That is quite impossible in the real world.

BTW, I cannot understand where you are heading with all

this nonsense about the LT.

You do understand that the LT explains the MMX just fine.

Or don't you?

MLuttgens (new):

The LT does not explain the MMX fine.

I claim

- that the negative result of the MMX can only mean

that light took the same time to travel (round-trip) the two legs,

- that a simple geometrical analysis shows that

t(perpendicular) = (2L/c) / sqrt(1 - (v/c)^2), and

t(parallel) = (2L/c) / (1 - (v/c)^2),

- that those two round-trip times can only be equal if the time

along the parallel leg is slowed by a factor sqrt(1 - (v/c)^2),

and becomes

t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2), thus

t(parallel) = (2L/c) / sqrt(1 - (v/c)^2),

= t(perpendicular),

meaning that clock slowing in the direction parallel to motion

suffices to explain the "null" result of the MMX,

- that clock slowing is a well attested phenomenon (GPS,

Haefele and Keating, etc...), whereas physical length contraction

has never been experimentally observed,

- that the fact that the formula giving t(parallel) can be written

t(parallel) = (2L*sqrt(1-(v/c)^2) / c[1 - (v/c)^2]) is not a proof of

length contraction, but must be considered as a mere

mathematical "artefact".

- that, consequently, the correct LT is

x' = x y' = y

t' = gamma * (t - vx / c^2), with gamma = 1/sqrt(1 - (v/c)^2),

and the "general" LT is, assuming that a is the angle

between arm and velocity vector, measured in the interferometer

frame, and v*cos(a) is the relevant velocity:

x' = x y' = y

t' = gamma * (t - v*cos(a)*x / c^2),

with gamma = 1/sqrt(1 - (v*cos(a))^2)/c^2)

Indeed, as there is no physical length contraction, the angle a

is constant ( = frame independent), and neither y nor x are

modified.

- that a general geometrical analysis of the MMX leads to the

formula t = (2L/c*(1-v^2)) * sqrt(1 - ((v/c)*sin(a))^2), giving

the round-trip travel time of light when time slowing is not

taken into consideration, and to the formula

t = (2L/c*(1-(v/c)^2)) * sqrt(1 - ((v/c)*sin(a))^2) *

sqrt(1 - ((v/c)*cos(a))^2)

when the clock slowing factor

sqrt(1 - ((v/c)*cos(a))^2) is applied.

Note that *without* time slowing, we get

for the perpendicular arm (sin(a)=1):

t = (2L/c*(1-(v/c)^2)) * sqrt(1 - (v/c)^2)

= (2L/c) / sqrt(1 - (v/c)^2), which is the same formula

as above,

and for the parallel arm (sin(a)=0):

t = (2L/c) / (1-(v/c)^2), again the same formula as above.

But *with* time slowing, by multiplying those times by the

factor sqrt(1 - ((v/c)*cos(a))^2), we obtain

for the perpendicular arm (cos(a)=0):

t = (2L/c) / sqrt(1 - (v/c)^2),

and for the parallel arm (cos(a)=1):

t = ((2L/c) / (1-(v/c)^2)) * sqrt(1-(v/c)^2)

= (2L/c) / sqrt(1 - (v/c)^2),

thus identical times for both arms.

Btw, I dont find any pertinence to your remark

"There is only in a fantasy world that coinciding events are

not coinciding in every frame of reference".

Marcel Luttgens

Aug 17, 1999, 3:00:00 AM8/17/99

to

MLuttgens wrote:

>

> The LT does not explain the MMX fine.

>

> I claim

>

> - that the negative result of the MMX can only mean

> that light took the same time to travel (round-trip) the two legs,

>

> The LT does not explain the MMX fine.

>

> I claim

>

> - that the negative result of the MMX can only mean

> that light took the same time to travel (round-trip) the two legs,

Right.

> - that a simple geometrical analysis shows that

> t(perpendicular) = (2L/c) / sqrt(1 - (v/c)^2), and

> t(parallel) = (2L/c) / (1 - (v/c)^2),

According to the Galilean transformation, right.

> - that those two round-trip times can only be equal if the time

> along the parallel leg is slowed by a factor sqrt(1 - (v/c)^2),

> and becomes

> t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2), thus

> t(parallel) = (2L/c) / sqrt(1 - (v/c)^2),

> = t(perpendicular),

> meaning that clock slowing in the direction parallel to motion

> suffices to explain the "null" result of the MMX,

Still nonsense.

This inevitably leads to that coinciding events are

not coinciding in all frames.

I find it impossible to understand why it is not

obvious to you that this is impossible.

> - that clock slowing is a well attested phenomenon (GPS,

> Haefele and Keating, etc...), whereas physical length contraction

> has never been experimentally observed,

The consequences of length contraction is observed.

> - that the fact that the formula giving t(parallel) can be written

> t(parallel) = (2L*sqrt(1-(v/c)^2) / c[1 - (v/c)^2]) is not a proof of

> length contraction, but must be considered as a mere

> mathematical "artefact".

But that's what it is.

You cannot explain it without length contraction.

> - that, consequently, the correct LT is

>

> x' = x y' = y

> t' = gamma * (t - vx / c^2), with gamma = 1/sqrt(1 - (v/c)^2),

Funny claim.

That transformation predicts fringe shifts in the MMX.

Was it not the MMX you wanted to explain?

> and the "general" LT is, assuming that a is the angle

> between arm and velocity vector, measured in the interferometer

> frame, and v*cos(a) is the relevant velocity:

>

> x' = x y' = y

> t' = gamma * (t - v*cos(a)*x / c^2),

> with gamma = 1/sqrt(1 - (v*cos(a))^2)/c^2)

Even funnier. :-)

How can a co-ordinate transformation depend on

of the orientation of some rod?

The speed of light in a frame will depend on

the orientation of your rod.

Funny place, that dream world of yours. :-)

> Indeed, as there is no physical length contraction, the angle a

> is constant ( = frame independent), and neither y nor x are

> modified.

Right.

But your transformation will predict a number of things

which is not observed.

Like non invariant speed of light.

> - that a general geometrical analysis of the MMX leads to the

> formula t = (2L/c*(1-v^2)) * sqrt(1 - ((v/c)*sin(a))^2), giving

> the round-trip travel time of light when time slowing is not

> taken into consideration, and to the formula

> t = (2L/c*(1-(v/c)^2)) * sqrt(1 - ((v/c)*sin(a))^2) *

> sqrt(1 - ((v/c)*cos(a))^2)

> when the clock slowing factor

> sqrt(1 - ((v/c)*cos(a))^2) is applied.

>

> Note that *without* time slowing, we get

> for the perpendicular arm (sin(a)=1):

> t = (2L/c*(1-(v/c)^2)) * sqrt(1 - (v/c)^2)

> = (2L/c) / sqrt(1 - (v/c)^2), which is the same formula

> as above,

> and for the parallel arm (sin(a)=0):

> t = (2L/c) / (1-(v/c)^2), again the same formula as above.

>

> But *with* time slowing, by multiplying those times by the

> factor sqrt(1 - ((v/c)*cos(a))^2), we obtain

> for the perpendicular arm (cos(a)=0):

> t = (2L/c) / sqrt(1 - (v/c)^2),

> and for the parallel arm (cos(a)=1):

> t = ((2L/c) / (1-(v/c)^2)) * sqrt(1-(v/c)^2)

> = (2L/c) / sqrt(1 - (v/c)^2),

> thus identical times for both arms.

But it is impossible nonsense.

> Btw, I dont find any pertinence to your remark

> "There is only in a fantasy world that coinciding events are

> not coinciding in every frame of reference".

Don't you?

I think the pertinence of that remark should be blatantly

obvious. I have explained it before.

In the rod frame, the light paths are equal, and the two light

beams which are emitted as coinciding events, will hit the end

of the rods as coinciding events.

But without length contraction, the light paths in the "ether frame"

will be different. Thus the light will not hit the other end

of the rod as coinciding events. This is self contradictory nonsense,

which cannot be patched by demanding that the two light beams should

be timed by clocks running at different rates.

Which in any case is impossible nonsense.

Both light beams can in principle be timed by one single

clock at the intersection of the arms. The two light beams will

not hit this clock as coinciding events. Now you demand that

this clock shall run at two different rates - one rate for each

beam - and thus find that the beams use the same time.

I find it hard to understand how anybody can claim something

so utterly impossible and self contradicting.

I think I now am fed up with stating the obvious.

Paul

Aug 18, 1999, 3:00:00 AM8/18/99

to

In article <37B9DB97...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>

>MLuttgens wrote:

>>

>> The LT does not explain the MMX fine.

>>

>> I claim

>>

>> - that the negative result of the MMX can only mean

>> that light took the same time to travel (round-trip) the two legs,

>

>Right.

>

>> - that a simple geometrical analysis shows that

>> t(perpendicular) = (2L/c) / sqrt(1 - (v/c)^2), and

>> t(parallel) = (2L/c) / (1 - (v/c)^2),

>

>According to the Galilean transformation, right.

>

>> - that those two round-trip times can only be equal if the time

>> along the parallel leg is slowed by a factor sqrt(1 - (v/c)^2),

>> and becomes

>> t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2), thus

>> t(parallel) = (2L/c) / sqrt(1 - (v/c)^2),

>> = t(perpendicular),

>> meaning that clock slowing in the direction parallel to motion

>> suffices to explain the "null" result of the MMX,

>

>Still nonsense.

>This inevitably leads to that coinciding events are

>not coinciding in all frames.

>I find it impossible to understand why it is not

>obvious to you that this is impossible.

>

You are the one who is spouting nonsense.

Don't you realize that

1) t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2),

which explains the negative result of the MMX is terms

of time slowing, is strictly equivalent to

2) t(parallel) = [(2L * sqrt(1 - (v/c)^2)] / c) / (1 - (v/c)^2),

which explains the null result by a contraction of the arm's

length L by the factor sqrt(1 - (v/c)^2).

Or you accept the form 2), but reject its mathematically

equivalent form 1), because, according to you, it "leads to that

coinciding events are not coinciding in all frames".

If your objection were pertinent, it *should* apply to

both forms.

Moreover, as I said many times, time slowing has been

experimentally demonstrated, but never length contraction.

As you are obviously impervious to logical thinking, I take

no further interest in such discussion.

Marcel Luttgens

Aug 18, 1999, 3:00:00 AM8/18/99

to

MLuttgens wrote:

>

> In article <37B9DB97...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >

>

> In article <37B9DB97...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >

> >MLuttgens wrote:

> >>

> >> The LT does not explain the MMX fine.

> >>

> >> I claim

> >>

> >> - that the negative result of the MMX can only mean

> >> that light took the same time to travel (round-trip) the two legs,

> >

> >Right.

> >

> >> - that a simple geometrical analysis shows that

> >> t(perpendicular) = (2L/c) / sqrt(1 - (v/c)^2), and

> >> t(parallel) = (2L/c) / (1 - (v/c)^2),

> >

> >According to the Galilean transformation, right.

> >

> >> - that those two round-trip times can only be equal if the time

> >> along the parallel leg is slowed by a factor sqrt(1 - (v/c)^2),

> >> and becomes

> >> t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2), thus

> >> t(parallel) = (2L/c) / sqrt(1 - (v/c)^2),

> >> = t(perpendicular),

> >> meaning that clock slowing in the direction parallel to motion

> >> suffices to explain the "null" result of the MMX,

> >

> >Still nonsense.

> >This inevitably leads to that coinciding events are

> >not coinciding in all frames.

> >I find it impossible to understand why it is not

> >obvious to you that this is impossible.

> >

>

> >>

> >> The LT does not explain the MMX fine.

> >>

> >> I claim

> >>

> >> - that the negative result of the MMX can only mean

> >> that light took the same time to travel (round-trip) the two legs,

> >

> >Right.

> >

> >> - that a simple geometrical analysis shows that

> >> t(perpendicular) = (2L/c) / sqrt(1 - (v/c)^2), and

> >> t(parallel) = (2L/c) / (1 - (v/c)^2),

> >

> >According to the Galilean transformation, right.

> >

> >> - that those two round-trip times can only be equal if the time

> >> along the parallel leg is slowed by a factor sqrt(1 - (v/c)^2),

> >> and becomes

> >> t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2), thus

> >> t(parallel) = (2L/c) / sqrt(1 - (v/c)^2),

> >> = t(perpendicular),

> >> meaning that clock slowing in the direction parallel to motion

> >> suffices to explain the "null" result of the MMX,

> >

> >Still nonsense.

> >This inevitably leads to that coinciding events are

> >not coinciding in all frames.

> >I find it impossible to understand why it is not

> >obvious to you that this is impossible.

> >

>

> You are the one who is spouting nonsense.

> Don't you realize that

> 1) t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2),

> which explains the negative result of the MMX is terms

> of time slowing, is strictly equivalent to

> 2) t(parallel) = [(2L * sqrt(1 - (v/c)^2)] / c) / (1 - (v/c)^2),

> which explains the null result by a contraction of the arm's

> length L by the factor sqrt(1 - (v/c)^2).

>

> Or you accept the form 2), but reject its mathematically

> equivalent form 1), because, according to you, it "leads to that

> coinciding events are not coinciding in all frames".

> If your objection were pertinent, it *should* apply to

> both forms.

> Don't you realize that

> 1) t(parallel) = [(2L/c) / (1 - (v/c)^2)] * sqrt(1 - (v/c)^2),

> which explains the negative result of the MMX is terms

> of time slowing, is strictly equivalent to

> 2) t(parallel) = [(2L * sqrt(1 - (v/c)^2)] / c) / (1 - (v/c)^2),

> which explains the null result by a contraction of the arm's

> length L by the factor sqrt(1 - (v/c)^2).

>

> Or you accept the form 2), but reject its mathematically

> equivalent form 1), because, according to you, it "leads to that

> coinciding events are not coinciding in all frames".

> If your objection were pertinent, it *should* apply to

> both forms.

Of course the two forms are mathematically equivalent.

That is not the issue.

The point is that your theory is self contradictory.

> Moreover, as I said many times, time slowing has been

> experimentally demonstrated, but never length contraction.

> As you are obviously impervious to logical thinking, I take

> no further interest in such discussion.

>

> Marcel Luttgens

To state what should be blatantly obvious to anybody

not impervious to logical thinking yet again:

Consider this:

According to you (with no rod shortening), the path lengths

in the ether frame for the light going along the two beams are:

Parallel arm: LPp = L/(1 - v^2/c^2)

Transverse arm: LPt = L/sqrt(1 - v^2/c^2)

that means that if the light fronts start at ether time t = 0,

they will get back to the intersections of the arms at the

ether times:

Parallel arm: tp = 2*(L/c)/(1 - v^2/c^2)

Transverse arm: tt = 2*(L/c)/sqrt(1 - v^2/c^2)

that means that the events are not coinciding.

When the instrument is rotated 90 degrees, the times

will be interchanged.

Hence this theory predicts fringe shifts for the MMX

when the calculations are carried out in the ether frame.

So let's time them with a clock moving along with the interferometer.

This can obviously be done with a single clock at the intersections

of the arms, where all the relevant events take place.

This clock show t' = 0 when the lightfronts starts.

Now, according to you, this single clock must run at

the rate (1 - (v/c)^2) relative to ether time to

yield the time along the parallel arm:

tp' = [(2L/c) / (1 - (v/c)^2)] * (1 - (v/c)^2) = 2L/c

while it must run at the rate sqrt(1 - (v/c)^2) to yield

the time along the transverse arm:

tp' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c

How can you make this single clock run at two different rates

at the same time?

I have asked you this question a couple of times before,

but you have snipped it without comment every time.

Will you face it this time, or will you yet again snip

it without comment because I am "obviously impervious to

logical thinking"?

I expect the latter.

Prove me wrong!

Paul

Aug 18, 1999, 3:00:00 AM8/18/99

to

In article <37BAB5FE...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>Date : Wed, 18 Aug 1999 14:32:46 +0100

>

>MLuttgens wrote:

>

> In article <37B9DB97...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

[snip]

>So let's time them with a clock moving along with the interferometer.

>This can obviously be done with a single clock at the intersections

>of the arms, where all the relevant events take place.

>This clock show t' = 0 when the lightfronts starts.

>Now, according to you, this single clock must run at

>the rate (1 - (v/c)^2) relative to ether time to

>yield the time along the parallel arm:

> tp' = [(2L/c) / (1 - (v/c)^2)] * (1 - (v/c)^2) = 2L/c

>while it must run at the rate sqrt(1 - (v/c)^2) to yield

>the time along the transverse arm:

> tp' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c

>

>How can you make this single clock run at two different rates

>at the same time?

>

>I have asked you this question a couple of times before,

>but you have snipped it without comment every time.

>

>Will you face it this time, or will you yet again snip

>it without comment because I am "obviously impervious to

>logical thinking"?

>

>I expect the latter.

>Prove me wrong!

>

How could the interferometer's clock run at two different rates

at the same time?

According to everybody, it slows down by sqrt(1 - (v/c)^2)

wrt a clock at rest.

If, as you are claiming, the time slowing explanation of the

MMX's negative result is invalid, so must be the length

contraction one, because it relies on the same equation.

So, how do you explain, with your moving clock, that the rod

shrinking analysis is contradiction free?

Anyhow, suppose that 2L/c = 1 and that v = 0.6 c.

The observer at rest in the ether will see that the lightfront

travelling along the transverse arm took, according to his

clock, tt = 2L/c / sqrt(1 - (v/c)^2) = 1.25 s to come back

at the arms' intersection, against tp = 2L/c / (1 - (v/c)^2) =

1.5625 s for the the "parallel" lightfront. It is important to

note that this time difference has absolutely nothing to do

with the physical reality of the meeting of the lightfronts

at the intersection. This is precisely the origin of your

persistent error: a confusion between observation and reality.

Knowing that such time difference can only be explained by

the motion of the interferometer through the ether, the clever

observer will even calculate v from the expression sqrt (1-v^2) =

1.25 / 1.5625 = .8, and find that v = 0.6.

>Paul

Marcel Luttgens

Aug 18, 1999, 3:00:00 AM8/18/99

to

MLuttgens wrote:

>

> In article <37BAB5FE...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >Date : Wed, 18 Aug 1999 14:32:46 +0100

> >

> >MLuttgens wrote:

> >

> > In article <37B9DB97...@hia.no>, "Paul B. Andersen"

> > <paul.b....@hia.no> wrote :

> >

>

> [snip]

>

> >So let's time them with a clock moving along with the interferometer.

> >This can obviously be done with a single clock at the intersections

> >of the arms, where all the relevant events take place.

> >This clock show t' = 0 when the lightfronts starts.

> >Now, according to you, this single clock must run at

> >the rate (1 - (v/c)^2) relative to ether time to

> >yield the time along the parallel arm:

> > tp' = [(2L/c) / (1 - (v/c)^2)] * (1 - (v/c)^2) = 2L/c

> >while it must run at the rate sqrt(1 - (v/c)^2) to yield

> >the time along the transverse arm:

> > tt' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c>

> In article <37BAB5FE...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >Date : Wed, 18 Aug 1999 14:32:46 +0100

> >

> >MLuttgens wrote:

> >

> > In article <37B9DB97...@hia.no>, "Paul B. Andersen"

> > <paul.b....@hia.no> wrote :

> >

>

> [snip]

>

> >So let's time them with a clock moving along with the interferometer.

> >This can obviously be done with a single clock at the intersections

> >of the arms, where all the relevant events take place.

> >This clock show t' = 0 when the lightfronts starts.

> >Now, according to you, this single clock must run at

> >the rate (1 - (v/c)^2) relative to ether time to

> >yield the time along the parallel arm:

> > tp' = [(2L/c) / (1 - (v/c)^2)] * (1 - (v/c)^2) = 2L/c

> >while it must run at the rate sqrt(1 - (v/c)^2) to yield

> >the time along the transverse arm:

> >

> >How can you make this single clock run at two different rates

> >at the same time?

> >

> >I have asked you this question a couple of times before,

> >but you have snipped it without comment every time.

> >

> >Will you face it this time, or will you yet again snip

> >it without comment because I am "obviously impervious to

> >logical thinking"?

> >

> >I expect the latter.

> >Prove me wrong!

> >

>

> How could the interferometer's clock run at two different rates

> at the same time?

> According to everybody, it slows down by sqrt(1 - (v/c)^2)

> wrt a clock at rest.

So you have changed your mind? The clock run at only one rate?

In that case the predictions of your theory are:

The light fronts hit the end of the rods at the times

in the rod frame:

tp' = [(2L/c)/(1-(v/c)^2)]*sqrt(1-(v/c)^2) = (2L/c)/sqrt(1-(v/c)^2)

tt' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c

They does not hit the end of the rod as coinciding events.

So your theory predict fringe shifts.

Clock slowing alone cannot predict a null-result.

> If, as you are claiming, the time slowing explanation of the

> MMX's negative result is invalid, so must be the length

> contraction one, because it relies on the same equation.

SR has both time slowing and rod contraction.

I never said time slowing was impossible.

I said that two different slowings of a single clock

at the same time is impossible.

But it is the rod shortening that explains the MMX.

A theory with no time slowing, like Lorentz first theory

could explain it just fine.

A theory with time slowing alone can not,

as you so thoroughly if involuntarily have demonstrated.

> So, how do you explain, with your moving clock, that the rod

> shrinking analysis is contradiction free?

The simple point is that two rods which are differently

oriented relative to the velocity vector can shrink

differently, but you cannot make a single clock run

at two different rates at the same time.

If you do not see the difference between those,

you must be blind.

> Anyhow, suppose that 2L/c = 1 and that v = 0.6 c.

> The observer at rest in the ether will see that the lightfront

> travelling along the transverse arm took, according to his

> clock, tt = 2L/c / sqrt(1 - (v/c)^2) = 1.25 s to come back

> at the arms' intersection, against tp = 2L/c / (1 - (v/c)^2) =

> 1.5625 s for the the "parallel" lightfront. It is important to

> note that this time difference has absolutely nothing to do

> with the physical reality of the meeting of the lightfronts

> at the intersection.

So what are you talking about? A dream world?

I am talking about the real world.

> This is precisely the origin of your

> persistent error: a confusion between observation and reality.

If the light fronts are observed not to meet in coinciding

events, then they really don't do so.

You cannot make that an error by persistently claiming

the impossible.

> Knowing that such time difference can only be explained by

> the motion of the interferometer through the ether, the clever

> observer will even calculate v from the expression sqrt (1-v^2) =

> 1.25 / 1.5625 = .8, and find that v = 0.6.

Sure. But that does not make the events co-incide.

But all this evasive talk is rather mute now, isn't it?

You admitted above that the the moving clock and thus the time

in the interferometer frame can only run at one rate

relative to the ether time, and not at one rate for each

differently oriented rod you might have in that frame.

So it should be settled that time dilation alone cannot

predict a null result of the MMX.

Right?

Paul

Aug 19, 1999, 3:00:00 AM8/19/99

to

In article <37BB2888...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>Date : Wed, 18 Aug 1999 22:41:28 +0100

I never claimed that a clock can simultaneously run at two

different rates!

>In that case the predictions of your theory are:

>The light fronts hit the end of the rods at the times

>in the rod frame:

> tp' = [(2L/c)/(1-(v/c)^2)]*sqrt(1-(v/c)^2) = (2L/c)/sqrt(1-(v/c)^2)

> tt' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c

>They does not hit the end of the rod as coinciding events.

>So your theory predict fringe shifts.

>Clock slowing alone cannot predict a null-result.

>

No, my theory (?) predicts

tp' = (2L/c)/(1-(v/c)^2) *sqrt(1-(v/c)^2) = (2L/c)/sqrt(1-(v/c)^2)

tt' = (2L/c)/sqrt(1 - (v/c)^2) * 1 = (2L/c)/sqrt(1-(v/c)^2)

But I admit that the clock at the arms' intersection poses problem.

And you predict

tp' = (2L*sqrt(1-(v/c)^2) / c) / (1-(v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

tt' = (2L * 1 / c) / sqrt(1 - (v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

How simple!

But herunder, you accept that "SR has both time slowing and

rod contraction".

How do you integrate time slowing in your above formulae?

Do you just multiply tp' and tt' by sqrt(1-(v/c)^2), and obtain

2L/c in both cases?

But then, you would imply that time slowing affects the transverse

arm (supposed to be oriented at 90° wrt the velocity vector),

in contradiction with SR itself. And if you consider that

time slowing is limited to the parallel arm, you also face the

problem of a single clock running at two different rates at the

same time.

>> If, as you are claiming, the time slowing explanation of the

>> MMX's negative result is invalid, so must be the length

>> contraction one, because it relies on the same equation.

>

>SR has both time slowing and rod contraction.

Then SR is flawed, because both cannot exist at the same time.

You have to chose your solution, either time slowing or length

contraction.

>I never said time slowing was impossible.

>I said that two different slowings of a single clock

>at the same time is impossible.

>

>But it is the rod shortening that explains the MMX.

>A theory with no time slowing, like Lorentz first theory

>could explain it just fine.

Lorentz ignored that there *is* time slowing on rods oriented

at an angle other than 90° wrt the velocity vector. *You* cannot

neglect that fact.

>A theory with time slowing alone can not,

>as you so thoroughly if involuntarily have demonstrated.

>

>> So, how do you explain, with your moving clock, that the rod

>> shrinking analysis is contradiction free?

>

>The simple point is that two rods which are differently

>oriented relative to the velocity vector can shrink

>differently, but you cannot make a single clock run

>at two different rates at the same time.

>

They can shrink differently, but as "SR has both time slowing

and rod contraction", you must add time slowing to your analysis,

and then, you have also the problem of the single clock.

If you consider only rod shrinking, you are at variance with SR,

and one can as well claim that you use in fact time slowing

in disguise.

[snip]

>Paul

Marcel Luttgens

Aug 20, 1999, 3:00:00 AM8/20/99

to

Yes, you implicitly did.

And repeat it below.

> >In that case the predictions of your theory are:

> >The light fronts hit the end of the rods at the times

> >in the rod frame:

> > tp' = [(2L/c)/(1-(v/c)^2)]*sqrt(1-(v/c)^2) = (2L/c)/sqrt(1-(v/c)^2)

> > tt' = [(2L/c)/sqrt(1 - (v/c)^2)] * sqrt(1 - (v/c)^2) = 2L/c

> >They does not hit the end of the rod as coinciding events.

> >So your theory predict fringe shifts.

> >Clock slowing alone cannot predict a null-result.

> >

>

> No, my theory (?) predicts

> tp' = (2L/c)/(1-(v/c)^2) *sqrt(1-(v/c)^2) = (2L/c)/sqrt(1-(v/c)^2)

> tt' = (2L/c)/sqrt(1 - (v/c)^2) * 1 = (2L/c)/sqrt(1-(v/c)^2)

See?

You say the clock at the same time must run at the rate sqrt(1-(v/c)^2)

and 1 relative to ether time.

> But I admit that the clock at the arms' intersection poses problem.

So you admit that your idea is impossible, but choose to ignore it?

> And you predict

> tp' = (2L*sqrt(1-(v/c)^2) / c) / (1-(v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

> tt' = (2L * 1 / c) / sqrt(1 - (v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

Yes, but these times are in the ether frame. (tp and tt).

In the interferometer frame the times will be:

tp' = 2L/c, tt' = 2L/c

> How simple!

> But herunder, you accept that "SR has both time slowing and

> rod contraction".

> How do you integrate time slowing in your above formulae?

> Do you just multiply tp' and tt' by sqrt(1-(v/c)^2), and obtain

> 2L/c in both cases?

Of course.

> But then, you would imply that time slowing affects the transverse

> arm (supposed to be oriented at 90° wrt the velocity vector),

> in contradiction with SR itself.

Of course it affects both events equally.

The point is that the two events "light from transverse arm

hit end of arm" and "light from rarallel arm hit end of arm"

are coinciding. They have equal temporal co-ordinate in all frames,

but what that co-ordinate is, depend on the frame.

The temporal co-ordinate is for both events (2L/c)/sqrt(1-(v/c)^2)

in the ether frame, and 2L/c in the interferometer frame.

> And if you consider that

> time slowing is limited to the parallel arm, you also face the

> problem of a single clock running at two different rates at the

> same time.

Indeed.

That's why time slowing is not "limited to one arm".

> >> If, as you are claiming, the time slowing explanation of the

> >> MMX's negative result is invalid, so must be the length

> >> contraction one, because it relies on the same equation.

> >

> >SR has both time slowing and rod contraction.

>

> Then SR is flawed, because both cannot exist at the same time.

> You have to chose your solution, either time slowing or length

> contraction.

And why cannot both exist at the same time, pray tell?

> >I never said time slowing was impossible.

> >I said that two different slowings of a single clock

> >at the same time is impossible.

> >

> >But it is the rod shortening that explains the MMX.

> >A theory with no time slowing, like Lorentz first theory

> >could explain it just fine.

>

> Lorentz ignored that there *is* time slowing on rods oriented

> at an angle other than 90° wrt the velocity vector. *You* cannot

> neglect that fact.

What the heck are you talking about?

In his first "contraction only" theory, Lorentz ignored

time slowing completely. That theory (or rather hypothesis) was

devised with the sole purpose of explaining the MMX, and

time slowing is irrelevant for that purpose.

In his 1904 theory, he had time slowing as well as contraction

because that was necessary to make Maxwell's equations invariant

when transformed.

But he never had the crazy idea that this time slowing

in any way was dependent on the orientation of the arms.

> >A theory with time slowing alone can not,

> >as you so thoroughly if involuntarily have demonstrated.

> >

> >> So, how do you explain, with your moving clock, that the rod

> >> shrinking analysis is contradiction free?

> >

> >The simple point is that two rods which are differently

> >oriented relative to the velocity vector can shrink

> >differently, but you cannot make a single clock run

> >at two different rates at the same time.

> >

>

> They can shrink differently, but as "SR has both time slowing

> and rod contraction", you must add time slowing to your analysis,

> and then, you have also the problem of the single clock.

Why is it a problem that the clock has to run at single rate?

> If you consider only rod shrinking, you are at variance with SR,

> and one can as well claim that you use in fact time slowing

> in disguise.

Right.

So that's why we don't do that. We have both.

Honestly, you seem very confused.

I find it very hard to figure out exactly what your

misconceptions really are.

Paul

Aug 21, 1999, 3:00:00 AM8/21/99

to

In article <37BD13C9...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>Date : Fri, 20 Aug 1999 09:37:29 +0100

The factor 1 only means that there is no time slowing along the

transverse arm.

>> But I admit that the clock at the arms' intersection poses problem.

>

>So you admit that your idea is impossible, but choose to ignore it?

>

I have a simple solution, i.e. the intersection clock is

irrelevant for the transverse case. What matters is not the arm,

but the light path.

When the light front travels some distance, the intersection

with its clock move along the x-axis, away from the light path.

Hence, what the clock still measures has no signification for

the determination of the transverse time tt'.

>> And you predict

>> tp' = (2L*sqrt(1-(v/c)^2) / c) / (1-(v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

>> tt' = (2L * 1 / c) / sqrt(1 - (v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

>

>Yes, but these times are in the ether frame. (tp and tt).

The times tp' are given by two different forms of the same

equation, and both forms give the same result, i.e.

(2L/c) / sqrt(1-(v/c)^2). Claiming that using one form justify length

contraction is no more that a semantical trick.

>In the interferometer frame the times will be:

> tp' = 2L/c, tt' = 2L/c

>

Yes, by applying the factor sqrt(1-(v/c)^2) twice !

>> How simple!

>> But herunder, you accept that "SR has both time slowing and

>> rod contraction".

>> How do you integrate time slowing in your above formulae?

>> Do you just multiply tp' and tt' by sqrt(1-(v/c)^2), and obtain

>> 2L/c in both cases?

>

>Of course.

>

>> But then, you would imply that time slowing affects the transverse

>> arm (supposed to be oriented at 90° wrt the velocity vector),

>> in contradiction with SR itself.

>

>Of course it affects both events equally.

>The point is that the two events "light from transverse arm

>hit end of arm" and "light from pararallel arm hit end of arm"

>are coinciding. They have equal temporal co-ordinate in all frames,

>but what that co-ordinate is, depend on the frame.

>The temporal co-ordinate is for both events (2L/c)/sqrt(1-(v/c)^2)

>in the ether frame, and 2L/c in the interferometer frame.

>

>> And if you consider that

>> time slowing is limited to the parallel arm, you also face the

>> problem of a single clock running at two different rates at the

>> same time.

>

>Indeed.

>That's why time slowing is not "limited to one arm".

>

In contradiction with SR !

>> >> If, as you are claiming, the time slowing explanation of the

>> >> MMX's negative result is invalid, so must be the length

>> >> contraction one, because it relies on the same equation.

>> >

>> >SR has both time slowing and rod contraction.

>>

>> Then SR is flawed, because both cannot exist at the same time.

>> You have to chose your solution, either time slowing or length

>> contraction.

>

>And why cannot both exist at the same time, pray tell?

>

>> >I never said time slowing was impossible.

>> >I said that two different slowings of a single clock

>> >at the same time is impossible.

>> >

>> >But it is the rod shortening that explains the MMX.

>> >A theory with no time slowing, like Lorentz first theory

>> >could explain it just fine.

>>

>> Lorentz ignored that there *is* time slowing on rods oriented

>> at an angle other than 90° wrt the velocity vector. *You* cannot

>> neglect that fact.

>

>What the heck are you talking about?

>In his first "contraction only" theory, Lorentz ignored

>time slowing completely.

That's what I meant.

>That theory (or rather hypothesis) was

>devised with the sole purpose of explaining the MMX, and

>time slowing is irrelevant for that purpose.

No, time slowing perfectly explains the MMX, you don't need

length contraction at all. As I just demonstrated above, the

intersection clock is a red herring.

>In his 1904 theory, he had time slowing as well as contraction

>because that was necessary to make Maxwell's equations invariant

>when transformed.

>But he never had the crazy idea that this time slowing

>in any way was dependent on the orientation of the arms.

>

>> >A theory with time slowing alone can not,

>> >as you so thoroughly if involuntarily have demonstrated.

>> >

>> >> So, how do you explain, with your moving clock, that the rod

>> >> shrinking analysis is contradiction free?

>> >

>> >The simple point is that two rods which are differently

>> >oriented relative to the velocity vector can shrink

>> >differently, but you cannot make a single clock run

>> >at two different rates at the same time.

>> >

>>

>> They can shrink differently, but as "SR has both time slowing

>> and rod contraction", you must add time slowing to your analysis,

>> and then, you have also the problem of the single clock.

>

>Why is it a problem that the clock has to run at single rate?

>

>> If you consider only rod shrinking, you are at variance with SR,

>> and one can as well claim that you use in fact time slowing

>> in disguise.

>

>Right.

>So that's why we don't do that. We have both.

>

Which is a physical nonsense.

>Honestly, you seem very confused.

>I find it very hard to figure out exactly what your

>misconceptions really are.

>

>Paul

Paul, your theory is false, I'm trying to convince you.

Consider an apparatus composed of two sources of

monochromatic light equidistant from a detector of interference

fringes. The length of arms 1 and 2 is L.

In the first case, the apparatus is perpendicular to the velocity

vector v. When the fronts arrive at the detector, t1 = t2 =

(L/c) / sqrt(1-(v/c)^2). Note that this result is obtained with

the help of the time slowing factor sqrt(1-(v/c)^2), that you

call arbitrarily a length contraction factor.

To get the times in the interferometer frame, you, as a smart

relativist, myltiply t1 and t2 by the time slowing factor sqrt(1-(v/c)^2,

and obtain t1' = t2' = L/c, a correct result according to SR.

In the second case, the apparatus is comoving with the velocity

vector, so, according to you, t1 = (L/(c-v)) * sqrt(1-(v/c)^2),

because of length contraction, and, similarly,

t2 = (L/(c+v)) * sqrt(1-(v/c)^2).

Now, again to get the interferometer times t1' and t2', you

multiply t1 and t2 a second time by sqrt(1-(v/c)^2), which you

now consider as a time slowing factor, and you obtain

t1' = (L/(c-v)) * (1-(v/c)^2) = (L/c) * (1+v/c), and

t2' = (L/(c+v)) * (1-(v/c)^2) = (L/c) * (1-v/c).

How do you explain that t1' and t2' are not only different from

L/c, but also that you get now interference fringes?

Do you still find SR a coherent and correct theory?

Marcel Luttgens

Aug 21, 1999, 3:00:00 AM8/21/99

to

Which is ridiculous.

> >> But I admit that the clock at the arms' intersection poses problem.

> >

> >So you admit that your idea is impossible, but choose to ignore it?

> >

>

> I have a simple solution, i.e. the intersection clock is

> irrelevant for the transverse case. What matters is not the arm,

> but the light path.

> When the light front travels some distance, the intersection

> with its clock move along the x-axis, away from the light path.

> Hence, what the clock still measures has no signification for

> the determination of the transverse time tt'.

:-)

Some proposals defies logic. This is one of them.

> >> And you predict

> >> tp' = (2L*sqrt(1-(v/c)^2) / c) / (1-(v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

> >> tt' = (2L * 1 / c) / sqrt(1 - (v/c)^2) = (2L/c) / sqrt(1-(v/c)^2)

> >

> >Yes, but these times are in the ether frame. (tp and tt).

>

> The times tp' are given by two different forms of the same

> equation, and both forms give the same result, i.e.

> (2L/c) / sqrt(1-(v/c)^2). Claiming that using one form justify length

> contraction is no more that a semantical trick.

I said this is the times in the ether frame.

How can that be a semantic trick?

> >In the interferometer frame the times will be:

> > tp' = 2L/c, tt' = 2L/c

> >

>

> Yes, by applying the factor sqrt(1-(v/c)^2) twice !

Sure.

But only once as time dilation.

> >> How simple!

> >> But herunder, you accept that "SR has both time slowing and

> >> rod contraction".

> >> How do you integrate time slowing in your above formulae?

> >> Do you just multiply tp' and tt' by sqrt(1-(v/c)^2), and obtain

> >> 2L/c in both cases?

> >

> >Of course.

> >

> >> But then, you would imply that time slowing affects the transverse

> >> arm (supposed to be oriented at 90° wrt the velocity vector),

> >> in contradiction with SR itself.

> >

> >Of course it affects both events equally.

> >The point is that the two events "light from transverse arm

> >hit end of arm" and "light from pararallel arm hit end of arm"

> >are coinciding. They have equal temporal co-ordinate in all frames,

> >but what that co-ordinate is, depend on the frame.

> >The temporal co-ordinate is for both events (2L/c)/sqrt(1-(v/c)^2)

> >in the ether frame, and 2L/c in the interferometer frame.

> >

> >> And if you consider that

> >> time slowing is limited to the parallel arm, you also face the

> >> problem of a single clock running at two different rates at the

> >> same time.

> >

> >Indeed.

> >That's why time slowing is not "limited to one arm".

> In contradiction with SR !

I hope you are joking, but fear you are confused.

I see you keep asserting.

> >In his 1904 theory, he had time slowing as well as contraction

> >because that was necessary to make Maxwell's equations invariant

> >when transformed.

> >But he never had the crazy idea that this time slowing

> >in any way was dependent on the orientation of the arms.

> >

> >> >A theory with time slowing alone can not,

> >> >as you so thoroughly if involuntarily have demonstrated.

> >> >

> >> >> So, how do you explain, with your moving clock, that the rod

> >> >> shrinking analysis is contradiction free?

> >> >

> >> >The simple point is that two rods which are differently

> >> >oriented relative to the velocity vector can shrink

> >> >differently, but you cannot make a single clock run

> >> >at two different rates at the same time.

> >> >

> >>

> >> They can shrink differently, but as "SR has both time slowing

> >> and rod contraction", you must add time slowing to your analysis,

> >> and then, you have also the problem of the single clock.

> >

> >Why is it a problem that the clock has to run at single rate?

> >

> >> If you consider only rod shrinking, you are at variance with SR,

> >> and one can as well claim that you use in fact time slowing

> >> in disguise.

> >

> >Right.

> >So that's why we don't do that. We have both.

> >

>

> Which is a physical nonsense.

Why?

> >Honestly, you seem very confused.

> >I find it very hard to figure out exactly what your

> >misconceptions really are.

> >

> >Paul

>

> Paul, your theory is false, I'm trying to convince you.

You mean SR is false.

> Consider an apparatus composed of two sources of

> monochromatic light equidistant from a detector of interference

> fringes. The length of arms 1 and 2 is L.

I suppose you mean like this:

S -> light D light <- S

|-----------|-----------|

L L

> In the first case, the apparatus is perpendicular to the velocity

> vector v. When the fronts arrive at the detector, t1 = t2 =

> (L/c) / sqrt(1-(v/c)^2). Note that this result is obtained with

> the help of the time slowing factor sqrt(1-(v/c)^2), that you

> call arbitrarily a length contraction factor.

You do not specify your examples wery well.

So I will have to guess.

The apparatus is moving perpendicular in the ether frame.

Your times t1 and t2 for the light to go from the sourse to

the detector are measured ** in the ether frame **.

There are neither any contraction nor time dilation in this

case of course. The length of the light pathes are

simply L/sqrt(1-(v/c)^2), and since the light is going with c,

the times must be as you say.

> To get the times in the interferometer frame, you, as a smart

> relativist, myltiply t1 and t2 by the time slowing factor sqrt(1-(v/c)^2,

> and obtain t1' = t2' = L/c, a correct result according to SR.

Right.

> In the second case, the apparatus is comoving with the velocity

> vector, so, according to you, t1 = (L/(c-v)) * sqrt(1-(v/c)^2),

> because of length contraction, and, similarly,

> t2 = (L/(c+v)) * sqrt(1-(v/c)^2).

I suppose you mean that the length axis of the apparatus is

parallel with the velocity, and that the light fronts are

both emitted at ether time t = 0,

e.g. *** sumultaneously in the ether frame. ***

In that case, your equations are correct.

Note that the times are different, e.g the two events

"hit detector" are not coinciding.

Rather obvious, since the detector moves.

In this scenario the two events are not coinciding.

===================================================

> Now, again to get the interferometer times t1' and t2', you

> multiply t1 and t2 a second time by sqrt(1-(v/c)^2), which you

> now consider as a time slowing factor, and you obtain

> t1' = (L/(c-v)) * (1-(v/c)^2) = (L/c) * (1+v/c), and

> t2' = (L/(c+v)) * (1-(v/c)^2) = (L/c) * (1-v/c).

Right.

> How do you explain that t1' and t2' are not only different from

> L/c, but also that you get now interference fringes?

Because it is correct.

In the "apparatus frame", the light fronts from the sources

are emitted at the _different_ times t01' and t02', where

t01' = Lv/c^2 and t02' = -Lv/c^2. Since the pulses both

use the time L/c on the journey, they will hit the detector

at the times:

t1' = Lv/c^2 + L/c = (L/c)*(1+v/c)

t2' = -Lv/c^2 + L/c = (L/c)*(1-v/c)

Of course the events are not coinciding.

SR would have been a pretty crazy theory if the events

which are not coinciding as described in your scenario

had been coinciding when transformed to the other frame.

Right?

Events are either coinciding or they are not.

In this case, they are not.

In any frame.

> Do you still find SR a coherent and correct theory?

Indeed.

But you have demonstrated your confusion yet again.

You are ascribing your failure to understand SR to

problems with SR.

Not uncommon, but the lack of self criticism that

displays always puzzles me.

Paul

Aug 23, 1999, 3:00:00 AM8/23/99

to

In article <37BEBBF1...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>Date : Sat, 21 Aug 1999 15:47:13 +0100

>

>MLuttgens wrote:

[snip]

>> I have a simple solution, etc...

>Some proposals defies logic. This is one of them.

>

Another solution that doesn't defy logic is that Michelson and

Morley were unable to detect fringe shifts, simply because they

are too small. Indeed, for arms of 11 m, a wavelength of

5.9E-5 cm, and a velocity v/c of 1E-4, we find

FRINGE SHIFTS:

Alpha= 30 9.322033689285912D-02

Alpha= 33.75 7.134776073470397D-02

Alpha= 37.5 4.825439608104603D-02

Alpha= 41.25 2.433539524511251D-02

Alpha= 45 0

Alpha= 48.75 -2.433539524511251D-02

Alpha= 52.5 -4.825439608104603D-02

Alpha= 56.25 -7.134776073470397D-02

Alpha= 60 -9.322033689285912D-02

N.B. : Alpha is the angle between one arm of the MM interferometer

and the velocity vector

The fringes are so small for angles between 30° and

60°, that it is doubtful that Michelson and Morley could

detect them.

The obvious conclusion is that length contraction is not

needed to explain their negative result.

[snip]

>> Consider an apparatus composed of two sources of

>> monochromatic light equidistant from a detector of interference

>> fringes. The length of arms 1 and 2 is L.

>

>I suppose you mean like this:

>

> S -> light D light <- S

> |-----------|-----------|

> L L

>

Yes

>> In the first case, the apparatus is perpendicular to the velocity

>> vector v. When the fronts arrive at the detector, t1 = t2 =

>> (L/c) / sqrt(1-(v/c)^2). Note that this result is obtained with

>> the help of the time slowing factor sqrt(1-(v/c)^2), that you

>> call arbitrarily a length contraction factor.

>

>You do not specify your examples wery well.

>So I will have to guess.

>The apparatus is moving perpendicular in the ether frame.

>Your times t1 and t2 for the light to go from the sourse to

>the detector are measured ** in the ether frame **.

>

You guessed correctly.

>There are neither any contraction nor time dilation in this

>case of course. The length of the light pathes are

>simply L/sqrt(1-(v/c)^2), and since the light is going with c,

>the times must be as you say.

>

In the interferometer frame, the length of the pathes are

of course L, hence L(ether frame) = L(interferometre frame) /

sqrt(1-(v/c)^2), or L(interferometer frame) = L(ether frame) *

sqrt(1-(v/c)^2), meaning that L, measured in the ether frame,

must be contracted by sqrt(1-(v/c)^2) to get the length of the

arm in the interferometer frame.

Congratulation, with the above thought experiment, you

have demonstrated that the detection of a preferred frame, i.e.

the ether, is possible with the help of a one-way interferometer.

[snip]

>Paul

Marcel Luttgens

Aug 23, 1999, 3:00:00 AM8/23/99

to

MLuttgens wrote:

>

> In article <37BEBBF1...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >Some proposals defies logic. This is one of them.

> >

>

>

> In article <37BEBBF1...@hia.no>, "Paul B. Andersen"

> <paul.b....@hia.no> wrote :

>

> >Date : Sat, 21 Aug 1999 15:47:13 +0100

> >

> >MLuttgens wrote:

>

> [snip]

>

> >> I have a simple solution, etc...> >

> >MLuttgens wrote:

>

> [snip]

>

> >Some proposals defies logic. This is one of them.

> >

>

> Another solution that doesn't defy logic is that Michelson and

> Morley were unable to detect fringe shifts, simply because they

> are too small. Indeed, for arms of 11 m, a wavelength of

> 5.9E-5 cm, and a velocity v/c of 1E-4, we find

>

> FRINGE SHIFTS:

>

> Alpha= 30 9.322033689285912D-02

> Alpha= 33.75 7.134776073470397D-02

> Alpha= 37.5 4.825439608104603D-02

> Alpha= 41.25 2.433539524511251D-02

> Alpha= 45 0

> Alpha= 48.75 -2.433539524511251D-02

> Alpha= 52.5 -4.825439608104603D-02

> Alpha= 56.25 -7.134776073470397D-02

> Alpha= 60 -9.322033689285912D-02

>

> N.B. : Alpha is the angle between one arm of the MM interferometer

> and the velocity vector

> The fringes are so small for angles between 30° and

> 60°, that it is doubtful that Michelson and Morley could

> detect them.

> The obvious conclusion is that length contraction is not

> needed to explain their negative result.

> Morley were unable to detect fringe shifts, simply because they

> are too small. Indeed, for arms of 11 m, a wavelength of

> 5.9E-5 cm, and a velocity v/c of 1E-4, we find

>

> FRINGE SHIFTS:

>

> Alpha= 30 9.322033689285912D-02

> Alpha= 33.75 7.134776073470397D-02

> Alpha= 37.5 4.825439608104603D-02

> Alpha= 41.25 2.433539524511251D-02

> Alpha= 45 0

> Alpha= 48.75 -2.433539524511251D-02

> Alpha= 52.5 -4.825439608104603D-02

> Alpha= 56.25 -7.134776073470397D-02

> Alpha= 60 -9.322033689285912D-02

>

> N.B. : Alpha is the angle between one arm of the MM interferometer

> and the velocity vector

> The fringes are so small for angles between 30° and

> 60°, that it is doubtful that Michelson and Morley could

> detect them.

> The obvious conclusion is that length contraction is not

> needed to explain their negative result.

What are you talking about?

They rotated the interferometer all the way around and looked for

the greatest shifts in the position of the fringes during the rotation.

So what are those angles above supposed to mean?

Again I find it amazing that you seem to believe that the great

experimentalists Michelson and Morley were plain stupid, and

did an elementary error which nobody but you have detected

during more than a century.

>

> [snip]

>

> >> Consider an apparatus composed of two sources of

> >> monochromatic light equidistant from a detector of interference

> >> fringes. The length of arms 1 and 2 is L.

> >

> >I suppose you mean like this:

> >

> > S -> light D light <- S

> > |-----------|-----------|

> > L L

> >

>

> Yes

>

> >> In the first case, the apparatus is perpendicular to the velocity

> >> vector v. When the fronts arrive at the detector, t1 = t2 =

> >> (L/c) / sqrt(1-(v/c)^2). Note that this result is obtained with

> >> the help of the time slowing factor sqrt(1-(v/c)^2), that you

> >> call arbitrarily a length contraction factor.

> >

> >You do not specify your examples wery well.

> >So I will have to guess.

> >The apparatus is moving perpendicular in the ether frame.

> >Your times t1 and t2 for the light to go from the sourse to

> >the detector are measured ** in the ether frame **.

> >

>

> You guessed correctly.

>

> >There are neither any contraction nor time dilation in this

> >case of course. The length of the light pathes are

> >simply L/sqrt(1-(v/c)^2), and since the light is going with c,

> >the times must be as you say.

> >

>

> In the interferometer frame, the length of the pathes are

> of course L, hence L(ether frame) = L(interferometre frame) /

> sqrt(1-(v/c)^2), or L(interferometer frame) = L(ether frame) *

> sqrt(1-(v/c)^2), meaning that L, measured in the ether frame,

> must be contracted by sqrt(1-(v/c)^2) to get the length of the

> arm in the interferometer frame.

No. No. No.

There is no contraction of a transversely moving arm.

The length of the arm remains L in the ether frame.

But since the arm is moving, the path length of the light

in the ether frame is of course longer than the arm,

it is L/sqrt(1 - v^2/c^2).

Isn't it about time you get this right, after so long time

and so many postings?

> Congratulation, with the above thought experiment, you

> have demonstrated that the detection of a preferred frame, i.e.

> the ether, is possible with the help of a one-way interferometer.

So you think so?

You mean you pick an arbitrary frame, call it the "ether frame",

emit the pulses _simultaneously_ in this frame, and you can

in principle measure the speed of the apparatus relative to

that "ether frame". Sure you can.

You can detect the frame **because you emitted the pulses

simultaneously in this frame.**

Paul

Aug 24, 1999, 3:00:00 AM8/24/99

to

In article <37C1C20C...@hia.no>, "Paul B. Andersen"

<paul.b....@hia.no> wrote :

<paul.b....@hia.no> wrote :

>Date : Mon, 23 Aug 1999 22:50:04 +0100

>

>MLuttgens wrote:

>>

>> In article <37BEBBF1...@hia.no>, "Paul B. Andersen"

>> <paul.b....@hia.no> wrote :

>>

>> >Date : Sat, 21 Aug 1999 15:47:13 +0100

>> >

>> >MLuttgens wrote:

[snip]

>> Another solution that doesn't defy logic is that Michelson and

>> Morley were unable to detect fringe shifts, simply because they

>> are too small.

[snip]

>What are you talking about?

>They rotated the interferometer all the way around and looked for

>the greatest shifts in the position of the fringes during the rotation.

>So what are those angles above supposed to mean?

>

>Again I find it amazing that you seem to believe that the great

>experimentalists Michelson and Morley were plain stupid, and

>did an elementary error which nobody but you have detected

>during more than a century.