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Greg Egan
Posted: Tue Jan 16, 2007 6:36 pm
Guest
In article <1168883430_1227@sicinfo3.epfl.ch>, harry
<harald.vanlintelButNotThis@epfl.ch> wrote:

Quote:
"Chalky" <chalkyspam@bleachboys.co.uk> wrote in message
news:1168758870.922068.265170@51g2000cwl.googlegroups.com...

[snip]

Quote:
All I want to know are the velocities of
all other schrapnel particles relative to any given one, as a function
of the dispersion angle theta of their trajectories, as measured in a
reference frame which is stationary relative to the source of the
explosion.

[snip]

It's strikingly simple. This relative velocity is sometimes called "closing
velocity", in order to stress that this is *not* the relative velocity of
frame transformations. You don't switch frames; the rules of vector addition
are the same for high speeds as for low speeds!
This should not be confused with "Galilean" versus "relativistic" speed
addition which happens in frame transformations. The confusion sometimes
arises because in classical mechanics the two are mathematically the
same -not so in relativistic physics. See also how Einstein used standard
vector mathematics inside the same paragraph 5 in which he derived the
relativisitc addition equation: there he mentions that the relative speed of
a moving point and a light ray in the original reference frame is simply
(c-v).

Harald

I parsed the OP's question very differently! Although it's clear that
he's measuring *theta* in the centre-of-mass frame of the explosion, I
thought he wanted the velocity of one piece of shrapnel *as measured in
the frame of another piece of shrapnel*.

Of course if he wants everything as measured in the centre-of-mass frame,
the whole problem's trivial, and he can subtract the 3-vectors in that
frame.

But the fact that he used the relativistic addition of velocities formula
in his original post made me think he was after an answer in the shrapnel
frame. To be clear, if he does what you're suggesting then he'll get
relative speeds of up to 2v for oppositely directed shrapnel. This is
the old "one spaceship goes at 0.9c to my left, and another goes at 0.9 c
to my right, so I see them separating at 1.8c". Which is perfectly true,
and if that really is what the OP wants, then he doesn't need relativity
at all.
Chalky
Posted: Thu Jan 18, 2007 2:32 am
Guest
Greg Egan wrote:

Quote:
In article <1168883430_1227@sicinfo3.epfl.ch>, harry
harald.vanlintelButNotThis@epfl.ch> wrote:

"Chalky" <chalkyspam@bleachboys.co.uk> wrote in message
news:1168758870.922068.265170@51g2000cwl.googlegroups.com...

[snip]

All I want to know are the velocities of
all other schrapnel particles relative to any given one, as a function
of the dispersion angle theta of their trajectories, as measured in a
reference frame which is stationary relative to the source of the
explosion.

[snip]

It's strikingly simple. This relative velocity is sometimes called "closing
velocity", in order to stress that this is *not* the relative velocity of
frame transformations. You don't switch frames; the rules of vector addition
are the same for high speeds as for low speeds!
This should not be confused with "Galilean" versus "relativistic" speed
addition which happens in frame transformations. The confusion sometimes
arises because in classical mechanics the two are mathematically the
same -not so in relativistic physics. See also how Einstein used standard
vector mathematics inside the same paragraph 5 in which he derived the
relativisitc addition equation: there he mentions that the relative speed of
a moving point and a light ray in the original reference frame is simply
(c-v).

Harald

I parsed the OP's question very differently! Although it's clear that
he's measuring *theta* in the centre-of-mass frame of the explosion, I
thought he wanted the velocity of one piece of shrapnel *as measured in
the frame of another piece of shrapnel*.

That is correct

Quote:
Of course if he wants everything as measured in the centre-of-mass frame,
the whole problem's trivial, and he can subtract the 3-vectors in that
frame.

No. That is not what I wanted

Quote:
But the fact that he used the relativistic addition of velocities formula
in his original post made me think he was after an answer in the shrapnel
frame.

Absolutely correct

Quote:
To be clear, if he does what you're suggesting then he'll get
relative speeds of up to 2v for oppositely directed shrapnel. This is
the old "one spaceship goes at 0.9c to my left, and another goes at 0.9 c
to my right, so I see them separating at 1.8c". Which is perfectly true,
and if that really is what the OP wants, then he doesn't need relativity
at all.

If that is true, I will not bother paying any further attention to
Harald's post.


Chalky
John (Liberty) Bell
Posted: Tue Feb 20, 2007 12:07 pm
Guest
On Jan 18, 12:32 pm, Chalky <chalkys...@bleachboys.co.uk> wrote:
Quote:
Greg Egan wrote:
In article <1168883430_1...@sicinfo3.epfl.ch>, harry
harald.vanlintelButNotT...@epfl.ch> wrote:

"Chalky" <chalkys...@bleachboys.co.uk> wrote in message
news:1168758870.922068.265170@51g2000cwl.googlegroups.com...

[snip]

All I want to know are the velocities of
all other schrapnel particles relative to any given one, as a function
of the dispersion angle theta of their trajectories, as measured in a
reference frame which is stationary relative to the source of the
explosion.

[snip]

It's strikingly simple. This relative velocity is sometimes called "closing
velocity", in order to stress that this is *not* the relative velocity of
frame transformations. You don't switch frames; the rules of vector addition
are the same for high speeds as for low speeds!
This should not be confused with "Galilean" versus "relativistic" speed
addition which happens in frame transformations. The confusion sometimes
arises because in classical mechanics the two are mathematically the
same -not so in relativistic physics. See also how Einstein used standard
vector mathematics inside the same paragraph 5 in which he derived the
relativisitc addition equation: there he mentions that the relative speed of
a moving point and a light ray in the original reference frame is simply
(c-v).

Harald

I parsed the OP's question very differently! Although it's clear that
he's measuring *theta* in the centre-of-mass frame of the explosion, I
thought he wanted the velocity of one piece of shrapnel *as measured in
the frame of another piece of shrapnel*.

That is correct

Of course if he wants everything as measured in the centre-of-mass frame,
the whole problem's trivial, and he can subtract the 3-vectors in that
frame.

No. That is not what I wanted

But the fact that he used the relativistic addition of velocities formula
in his original post made me think he was after an answer in the shrapnel
frame.

Absolutely correct

To be clear, if he does what you're suggesting then he'll get
relative speeds of up to 2v for oppositely directed shrapnel. This is
the old "one spaceship goes at 0.9c to my left, and another goes at 0.9 c
to my right, so I see them separating at 1.8c". Which is perfectly true,
and if that really is what the OP wants, then he doesn't need relativity
at all.

If that is true, I will not bother paying any further attention to
Harald's post.

Chalky- Hide quoted text -

- Show quoted text -

I have been giving this subject some further thought recently, given
that Chalky originally asked the SR question while some of us were
still struggling to define a simple inertial reference model of an
observable expanding universe, relative to which accelerating
expansion could be plotted (during a still eariler discussion over at
sci.astro.research). In practice, the Milne (empty) model of EFE is
used for that purpose by astronomers, and this can be tabulated for z
shift as a function of distance, simply by plugging Omega_Lamda = 0
and Omega_M =0 into, for example, Ned Wright's Cosmic calculator.
Admittedly, Chalky originally asked about z shift as a function of
dispersion angle, but this question could equally well have been asked
as a function of physical separation (or luminosity distance).

Now, if I understand the foundations of the theory correctly, when
Lambda and M are both set to zero, there should be no gravity and GR
thus approximates to SR, giving an inertial model of both the
expanding universe and, presumably, of exploding relativistic bombs
(when gravity is negligible), as the schrapnel velocity approaches c.

However, since I have arrived at this conclusion from a philosophical
perspective as opposed to rigorous mathematical analysis, informed
comments from others would be appreciated.

JLB
(Change John to Liberty to respond by email)
Uncle Al
Posted: Wed Feb 21, 2007 11:48 am
Guest
"John (Liberty) Bell" wrote:
Quote:

On Jan 18, 12:32 pm, Chalky <chalkys...@bleachboys.co.uk> wrote:
Greg Egan wrote:
In article <1168883430_1...@sicinfo3.epfl.ch>, harry
harald.vanlintelButNotT...@epfl.ch> wrote:

"Chalky" <chalkys...@bleachboys.co.uk> wrote in message
news:1168758870.922068.265170@51g2000cwl.googlegroups.com...

[snip]

All I want to know are the velocities of
all other schrapnel particles relative to any given one, as a function
of the dispersion angle theta of their trajectories, as measured in a
reference frame which is stationary relative to the source of the
explosion.

[snip]

It's strikingly simple. This relative velocity is sometimes called "closing
velocity", in order to stress that this is *not* the relative velocity of
frame transformations. You don't switch frames; the rules of vector addition
are the same for high speeds as for low speeds!
This should not be confused with "Galilean" versus "relativistic" speed
addition which happens in frame transformations. The confusion sometimes
arises because in classical mechanics the two are mathematically the
same -not so in relativistic physics. See also how Einstein used standard
vector mathematics inside the same paragraph 5 in which he derived the
relativisitc addition equation: there he mentions that the relative speed of
a moving point and a light ray in the original reference frame is simply
(c-v).

Harald

I parsed the OP's question very differently! Although it's clear that
he's measuring *theta* in the centre-of-mass frame of the explosion, I
thought he wanted the velocity of one piece of shrapnel *as measured in
the frame of another piece of shrapnel*.

That is correct

Of course if he wants everything as measured in the centre-of-mass frame,
the whole problem's trivial, and he can subtract the 3-vectors in that
frame.

No. That is not what I wanted

But the fact that he used the relativistic addition of velocities formula
in his original post made me think he was after an answer in the shrapnel
frame.

Absolutely correct

To be clear, if he does what you're suggesting then he'll get
relative speeds of up to 2v for oppositely directed shrapnel. This is
the old "one spaceship goes at 0.9c to my left, and another goes at 0.9 c
to my right, so I see them separating at 1.8c". Which is perfectly true,
and if that really is what the OP wants, then he doesn't need relativity
at all.

If that is true, I will not bother paying any further attention to
Harald's post.

Chalky- Hide quoted text -

- Show quoted text -

I have been giving this subject some further thought recently, given
that Chalky originally asked the SR question while some of us were
still struggling to define a simple inertial reference model of an
observable expanding universe, relative to which accelerating
expansion could be plotted (during a still eariler discussion over at
sci.astro.research). In practice, the Milne (empty) model of EFE is
used for that purpose by astronomers, and this can be tabulated for z
shift as a function of distance, simply by plugging Omega_Lamda = 0
and Omega_M =0 into, for example, Ned Wright's Cosmic calculator.
Admittedly, Chalky originally asked about z shift as a function of
dispersion angle, but this question could equally well have been asked
as a function of physical separation (or luminosity distance).

Now, if I understand the foundations of the theory correctly, when
Lambda and M are both set to zero, there should be no gravity and GR
thus approximates to SR, giving an inertial model of both the
expanding universe and, presumably, of exploding relativistic bombs
(when gravity is negligible), as the schrapnel velocity approaches c.

However, since I have arrived at this conclusion from a philosophical
perspective as opposed to rigorous mathematical analysis, informed
comments from others would be appreciated.

http://en.wikipedia.org/wiki/Redshift
Local redshift approximates Galilean (Doppler), cosmic redshfit is
relativistic (relativistic Doppler).

If the source is moving at right angles to the observer's line of
sight the Galilean formula predicts *no* spectral shift while the
relativistic formula *does* predict a spectral shift. This is
observed - transverse Doppler shift. This is why a Beckman
ultracentrifuge pulls a million gees but there are no associated
relativistic gravitational effects (e.g., slowing of radioactive decay
or radial Mossbauer redshift at the rotor's inner rim).

Gravitational redshift is GM/rc^2 where GM is Big G times the
gravitating body's mass, c is lightspeed and r is the radial climb up
or down the gravitational well. A million gees shrinks the Harvard
Tower experiment (Pound and Rebka)

http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/gratim.html

to 0.0226 mm climb (a hair is ~0.06 mm wide). There is no radial
redshift experimentally observed in an ultracentrifuge.

--
Uncle Al
http://www.mazepath.com/uncleal/
(Toxic URL! Unsafe for children and most mammals)
http://www.mazepath.com/uncleal/lajos.htm#a2
John (Liberty) Bell
Posted: Tue Feb 27, 2007 12:53 pm
Guest
On Feb 21, 9:48 pm, Uncle Al <Uncle...@hate.spam.net> wrote:
Quote:
"John (Liberty) Bell" wrote:

I have been giving this subject some further thought recently, given
that Chalky originally asked the SR question while some of us were
still struggling to define a simple inertial reference model of an
observable expanding universe, relative to which accelerating
expansion could be plotted (during a still eariler discussion over at
sci.astro.research). In practice, the Milne (empty) model of EFE is
used for that purpose by astronomers, and this can be tabulated for z
shift as a function of distance, simply by plugging Omega_Lamda = 0
and Omega_M =0 into, for example, Ned Wright's Cosmic calculator.
Admittedly, Chalky originally asked about z shift as a function of
dispersion angle, but this question could equally well have been asked
as a function of physical separation (or luminosity distance).

Now, if I understand the foundations of the theory correctly, when
Lambda and M are both set to zero, there should be no gravity and GR
thus approximates to SR, giving an inertial model of both the
expanding universe and, presumably, of exploding relativistic bombs
(when gravity is negligible), as the schrapnel velocity approaches c.

However, since I have arrived at this conclusion from a philosophical
perspective as opposed to rigorous mathematical analysis, informed
comments from others would be appreciated.

http://en.wikipedia.org/wiki/Redshift
Local redshift approximates Galilean (Doppler), cosmic redshfit is
relativistic (relativistic Doppler).

In the current context I imagine that you mean "special relativistic
Doppler" here, whereas there are many astrophysics sites which stress
that the cosmological redshift is a "different" general relativistic
effect. However, I am not completely convinced by this argument,
especially if one is considering the limiting case (Milne) general
relativistic solution, where the cosmological constant is zero, and
the mass is zero. This point is not totally academic as this is the
reference model against which astronomers plot the observable dynamics
of the accelerating expansion of the universe as well as the goodness
of fit of the various 'optimally tweaked' models of EFE.

Quote:
If the source is moving at right angles to the observer's line of
sight the Galilean formula predicts *no* spectral shift while the
relativistic formula *does* predict a spectral shift.

This is very true.

Quote:
This is
observed - transverse Doppler shift. This is why a Beckman
ultracentrifuge pulls a million gees but there are no associated
relativistic gravitational effects (e.g., slowing of radioactive decay
or radial Mossbauer redshift at the rotor's inner rim).

?? I don't get this. You SHOULD get slowing of clocks in a centrifuge,
precisely because the inner rim is moving fast relative to us. In
fact, Einstein used the rotating disc argument to derive a general
relativistic slowing of clocks in such a situation, special
relativistically. Whether you describe this as a special relativistic
effect relative to us, or a general relativistic effect relative to a
resident of the centrifuge would seem to be largely a question of
taste.

Quote:
Gravitational redshift is GM/rc^2 where GM is Big G times the
gravitating body's mass, c is lightspeed and r is the radial climb up
or down the gravitational well.

This statement is not general enough. A linearly accelerating observer
also observes gravitational redshift, within his accelerating
reference frame, due entirely to that acceleration.

Quote:
A million gees shrinks the Harvard
Tower experiment (Pound and Rebka)
http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/gratim.html
to 0.0226 mm climb (a hair is ~0.06 mm wide). There is no radial
redshift experimentally observed in an ultracentrifuge.

True. From within the centrifuge, it is observed as a gravitational
redshigt.

John.
Phillip Helbig---remove C
Posted: Wed Feb 28, 2007 2:54 am
Guest
In article <1172559521.623516.214080@k78g2000cwa.googlegroups.com>,
"John (Liberty) Bell" <john.bell@accelerators.co.uk> writes:

Quote:
In the current context I imagine that you mean "special relativistic
Doppler" here, whereas there are many astrophysics sites which stress
that the cosmological redshift is a "different" general relativistic
effect. However, I am not completely convinced by this argument,

The argument is simple. The Doppler formula has a velocity which can be
calculated from the redshift. If the cosmological redshift is a Doppler
redshift, then this velocity is independent of the cosmological
parameters (which do NOT appear in the Doppler formula). The only way
out of this is the meaningless tautological definition of a new type of
distance trivially given by the Doppler formula itself. In general, NO
cosmological distance (and there are many) has a temporal derivative
which results in the velocity calculated from the Doppler formula.

Quote:
especially if one is considering the limiting case (Milne) general
relativistic solution, where the cosmological constant is zero, and
the mass is zero. This point is not totally academic as this is the
reference model against which astronomers plot the observable dynamics
of the accelerating expansion of the universe

Some astronomers, not all. This model has no special physical
significance. Some things are mathematically easier to calculate in it.
It is a "reference model" only in a very limited sense.
John (Liberty) Bell
Posted: Tue Mar 06, 2007 3:48 am
Guest
On Feb 28, 12:54 pm, hel...@astro.multiCLOTHESvax.de (Phillip Helbig---
remove CLOTHES to reply) wrote:
Quote:
In article <1172559521.623516.214...@k78g2000cwa.googlegroups.com>,
"John (Liberty) Bell" <john.b...@accelerators.co.uk> writes:

especially if one is considering the limiting case (Milne) general
relativistic solution, where the cosmological constant is zero, and
the mass is zero. This point is not totally academic as this is the
reference model against which astronomers plot the observable dynamics
of the accelerating expansion of the universe

Some astronomers, not all.

Point accepted

Quote:
This model has no special physical
significance.

Well, it _should_ have special physical significance. With no mass,
and no Lambda, test points _should_ then obey the simple laws of
inertial physics (and SR). If not, there would seem to be something
seriously wrong with EFE since I understood that GR is supposed to
reduce to SR, in the absence of gravity and acceleration.

(I am now really confused about this)

John.
 
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