From: harald on
On Jun 30, 10:03 pm, va...(a)icmf.inf.cu wrote:
> In a recent thread we established that
>  “Centre of mass inertial frames are the unique ones in 1905
> Relativity”http://groups.google.com.cu/group/sci.physics.relativity/browse_frm/t...
> We can’t have two (or more) of them at the same time, because the
> bodies belonging to all of them determine a unique centre of mass
> inertial frame. As a result, in 1905 Relativity the moving system (MS)
> can be only a body (or subset) belonging to the body set of the unique
> inertial frame (the stationary system). The MS can be moving with any
> velocity compatible with the same laws valid in every inertial frame,
> not being then in general an inertial one.

As you (should) know by now, that's not true:

"Let us take a system of co-ordinates in which the equations of
Newtonian mechanics hold good. In order to render our presentation
more precise and to distinguish this system of co-ordinates verbally
from others which will be introduced hereafter, we call it the
``stationary system.'' [...] Theory of the Transformation of Co-
ordinates and Times from a Stationary System to another System in
Uniform Motion of Translation Relatively to the Former [..] the axes
of the moving system are [...] parallel to the axes of the stationary
system."

> See the example at the end
> of paragraph 4 of the 30Jun1905 Einstein’s paper (rotating Earth).

And which you cannot understand.

For the sake of others I copy-paste my recent clarifications to you
which you apparently also cannot understand (and I won't try anymore):

At the beginning of paragraph 2 in the 30Jun1905 paper, Einstein
writes:

“1. The laws by which the states of physical systems undergo change
are not affected, whether these changes of state be referred to the
one or the other of two systems of co-ordinates in uniform translatory
motion.”

Those changes of state stem from classical (Newtonian) theory,
and he referred to Newtonian coordinate systems. That he had such a
physical consideration of systems along with the mathematical one is
essential for understanding his paper, and the part about moving
clocks in particular.

Probably it's best to first discuss the predictions from the older,
classical theory for this case; and then you will probably immediately
understand the prediction with the new one.

First, take Newton's theory. You surely know that that theory
predicts
that uniform motion does not at all affect the rate of a clock as
determined in a "stationary" system; and as also Einstein emphasized,
the word "stationary" commonly doesn't mean anything special, it's
just a Newtonian system that we pick. Now take a clock that is moving
uniformly in another direction, starting with a physical
consideration.

Surely you understand that it has qualitatively the *same* state of
motion; the direction of motion cannot make a difference for the
prediction.

Thus logically, the same can be said for a clock that is moving along
a polygonal trajectory, since an infinitely quick change of direction
does not affect the indication of a good clock.

Mathematically this physical understanding can be verified by
performing Galilean transformations at the turning points: the
time t is of course the same when we shift our coordinates, while
the time t' that we locally read cannot be affected by our change
of ruler position (please think this over).

*If* we next assume that also acceleration has no effect on clock
rate,
then we can extrapolate (by simple integration) this result to a
circular trajectory. As a matter of fact, this is what always *was*
assumed by everyone, based on Newtonian mechanics.

Now take the new theory. This one has the following "physical
meaning":

"The time marked by [a uniformly moving] clock (viewed in the
stationary system) is slow by 1 - sqrt{1-v^2/c^2} seconds per
second."

Following the same *physical* logic as in the old theory, the
direction of motion cannot affect the physics; thus "It is at once
apparent that this result still holds good if the clock moves from
A to B in any polygonal line".

This can be verified mathematically (which takes a little longer than
the immediate physical insight based on state of motion) by performing
Lorentz transformations at the turning points. Then we verify that
when switching to another location, the time t remains of course the
same. Also the corresponding t' at that point (a physical event)
cannot be affected by our change of ruler position, as that would
contradict with what is observed with the first ruler position.

Next, "*If* we assume that the result proved for a polygonal line is
also valid for a continuously curved line", Einstein comes to his
prediction about a clock moving in a circular trajectory.

[NOTE: just as as the earlier, Newtonian prediction, that prediction
has nothing to do with confusing non-inertial frames with inertial
frames!]

Following that, he makes a prediction in which he lets go of his
overly simple example of Newtonian systems that are determined by
means of "stationary" clocks and rods on a fixed body;
instead he now refers to the ECI coordinate system which is in
nearly uniform motion but in which almost no reference matter is
perfectly in rest. As PD also pointed out, this was already well
understood in Newtonian mechanics and Einstein based himself on
the use of Newtonian reference systems.

Best regards,
Harald
From: artful on
On Jul 1, 6:03 am, va...(a)icmf.inf.cu wrote:
> In a recent thread we established that
>  “Centre of mass inertial frames are the unique ones in 1905
> Relativity”http://groups.google.com.cu/group/sci.physics.relativity/browse_frm/t...

That is just plain wrong. You may THINK you've established it, but
you have no idea.

Any inertial frame is fine. Nothing to do with any mass,

[snip rest of nonsense]
From: whoever on
>wrote in message
>news:cf9a3f56-d5ca-4a3e-8df9-29d3d626153c(a)5g2000yqz.googlegroups.com...
>
>On 30 jun, 15:13, stevendaryl3...(a)yahoo.com (Daryl McCullough) wrote:
>> va...(a)icmf.inf.cu says...
>>
>>
>>
>> >In a recent thread we established that
>> > Centre of mass inertial frames are the unique ones in 1905
>> >Relativity
>>
>> There is nothing in the development of relativity that in any
>> way depends on a frame being defined by a center of mass. That's
>> completely barking up the wrong tree.
>>
>> --
>> Daryl McCullough
>> Ithaca, NY
>
>I will answer you with the same initial post of the referred thread:

Repeating nonsense does not make it true

> [Let be any body set with a material point modelling each one.

OK .. so you start off with an ungrammatical sentence which makes no sense.

Try again

[snip more nonsense]


--- news://freenews.netfront.net/ - complaints: news(a)netfront.net ---
From: valls on
On 30 jun, 19:22, "whoever" <whoe...(a)whereever.com> wrote:
> >wrote in message
> >news:cf9a3f56-d5ca-4a3e-8df9-29d3d626153c(a)5g2000yqz.googlegroups.com...
>
> >On 30 jun, 15:13, stevendaryl3...(a)yahoo.com (Daryl McCullough) wrote:
> >> va...(a)icmf.inf.cu says...
>
> >> >In a recent thread we established that
> >> > Centre of mass inertial frames are the unique ones in 1905
> >> >Relativity
>
> >> There is nothing in the development of relativity that in any
> >> way depends on a frame being defined by a center of mass. That's
> >> completely barking up the wrong tree.
>
> >> --
> >> Daryl McCullough
> >> Ithaca, NY
>
> >I will answer you with the same initial post of the referred thread:
>
> Repeating nonsense does not make it true
>
> > [Let be any body set with a material point modelling each one.
>
> OK .. so you start off with an ungrammatical sentence which makes no sense.
>
> Try again
>
A body modelled by a material point is a very basic Newtonian concept.
Without it, the Newtonian mechanics laws have no sense at all. The
position of a body in some space at the corresponding instant of some
time, is the position of the material point modelling the body. Any
force acting in a body is a force acting in a straight line crossing
the material point modelling the body. The distance between two bodies
(to appy the gravitation law) is the distance between the material
points modelling the two bodies. You need more?
Try again.

RVHG (Rafael Valls Hidalgo-Gato)
From: valls on
On 30 jun, 18:12, artful <artful...(a)hotmail.com> wrote:
> On Jul 1, 6:03 am, va...(a)icmf.inf.cu wrote:
>
> > In a recent thread we established that
> >  “Centre of mass inertial frames are the unique ones in 1905
> > Relativity”http://groups.google.com.cu/group/sci.physics.relativity/browse_frm/t...
>
> That is just plain wrong.  You may THINK you've established it, but
> you have no idea.
>
> Any inertial frame is fine.  Nothing to do with any mass,
>
You forget that the topic in this thread is 1905 Relativity, where an
inertial frame, denoted by 1905 Einstein stationary system, is related
with mass without any doubt at all. To help you the understanding of
it, I will put here some text from the 30Jun1905 Einstein’s paper
(between [ ]):
Almost at the end of the Introduction: [The theory to be developed is
based –like all electrodynamics- on the kinematics of the rigid body,
since the assertions of any such theory have to do with the
relationships between rigid bodies (system of co-ordinates), clocks,
and electromagnetic processes.]. See here how 1905 Einstein identify
systems of co-ordinates with rigid bodies. Can you conceive a rigid
body without mass?
At the beginning of paragraph 2, where he defines “stationary system”:
[Let us take a system of co-ordinates in which the equation of
Newtonian mechanics hold good.]. A direct identification between
inertial system with massive system of co-ordinates.
At the beginning of paragraph 3: [Let us in “stationary space” take
two system of co-ordinates, i.e. two systems, each of three rigid
material lines, perpendicular to one another, and issuing from a
point.]. A single material point is already a massive entity, and we
have here RIGID MATERIAL LINES associated with the inertial frames. I
will suppose this is already sufficient for you to understand that to
talk about a non-massive inertial frame in 1905 Relativity is a
complete absurd.

RVHG (Rafael Valls Hidalgo-Gato)
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