On Sun, Sep 15, 2019 at 12:05 PM Alan Grayson <[email protected]>
wrote:

>
>
> On Sunday, September 15, 2019 at 9:58:53 AM UTC-6, Jason wrote:
>>
>>
>>
>> On Sun, Sep 15, 2019 at 7:36 AM Alan Grayson <[email protected]> wrote:
>>
>>>
>>>
>>> On Sunday, September 15, 2019 at 1:01:23 AM UTC-6, Jason wrote:
>>>>
>>>>
>>>>
>>>> On Sun, Sep 15, 2019 at 12:02 AM Alan Grayson <[email protected]>
>>>> wrote:
>>>>
>>>>>
>>>>>
>>>>> On Saturday, September 14, 2019 at 4:34:28 PM UTC-6, Jason wrote:
>>>>>>
>>>>>>
>>>>>>
>>>>>> On Sat, Sep 14, 2019 at 3:06 PM Alan Grayson <[email protected]>
>>>>>> wrote:
>>>>>>
>>>>>>>
>>>>>>>
>>>>>>> On Saturday, September 14, 2019 at 7:46:27 AM UTC-6, Jason wrote:
>>>>>>>>
>>>>>>>>
>>>>>>>>
>>>>>>>> On Sat, Sep 14, 2019, 4:36 AM Alan Grayson <[email protected]>
>>>>>>>> wrote:
>>>>>>>>
>>>>>>>>>
>>>>>>>>>
>>>>>>>>> On Saturday, September 14, 2019 at 12:34:18 AM UTC-6, Jason wrote:
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>> On Friday, September 13, 2019, Alan Grayson <[email protected]>
>>>>>>>>>> wrote:
>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>> On Friday, September 13, 2019 at 4:42:00 PM UTC-6, Jason wrote:
>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>> On Fri, Sep 13, 2019 at 8:25 AM Alan Grayson <
>>>>>>>>>>>> [email protected]> wrote:
>>>>>>>>>>>>
>>>>>>>>>>>>>
>>>>>>>>>>>>>
>>>>>>>>>>>>> On Friday, September 13, 2019 at 5:24:11 AM UTC-6, Bruno
>>>>>>>>>>>>> Marchal wrote:
>>>>>>>>>>>>>>
>>>>>>>>>>>>>>
>>>>>>>>>>>>>> On 13 Sep 2019, at 04:26, Alan Grayson <[email protected]>
>>>>>>>>>>>>>> wrote:
>>>>>>>>>>>>>>
>>>>>>>>>>>>>>
>>>>>>>>>>>>>>
>>>>>>>>>>>>>> On Thursday, September 12, 2019 at 11:01:54 AM UTC-6, Alan
>>>>>>>>>>>>>> Grayson wrote:
>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>> On Thursday, September 12, 2019 at 7:45:22 AM UTC-6,
>>>>>>>>>>>>>>> Lawrence Crowell wrote:
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>> On Thursday, September 12, 2019 at 4:20:46 AM UTC-5, Philip
>>>>>>>>>>>>>>>> Thrift wrote:
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>> On Wednesday, September 11, 2019 at 11:45:41 PM UTC-5,
>>>>>>>>>>>>>>>>> Alan Grayson wrote:
>>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>> https://www.wired.com/story/sean-carroll-thinks-we-all-exist-on-multiple-worlds/
>>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>> Many Worlds is where people go to escape from one world of
>>>>>>>>>>>>>>>>> quantum-stochastic processes. They are like vampires, but 
>>>>>>>>>>>>>>>>> instead of
>>>>>>>>>>>>>>>>> running away from sunbeams, are running away from 
>>>>>>>>>>>>>>>>> probabilities.
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>> @philipthrift
>>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>> This assessment is not entirely fair. Carroll and Sebens
>>>>>>>>>>>>>>>> have a paper on how supposedly the Born rule can be derived 
>>>>>>>>>>>>>>>> from MWI  I
>>>>>>>>>>>>>>>> have yet to read their paper, but given the newsiness of this 
>>>>>>>>>>>>>>>> I might get
>>>>>>>>>>>>>>>> to it. One advantage that MWI does have is that it splits the 
>>>>>>>>>>>>>>>> world as a
>>>>>>>>>>>>>>>> sort of quantum frame dragging that is nonlocal. This nonlocal 
>>>>>>>>>>>>>>>> property
>>>>>>>>>>>>>>>> might be useful for working with quantum gravity,
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>> I worked a proof of a theorem, which may not be complete
>>>>>>>>>>>>>>>> unfortunately, where the two sets of quantum interpretations 
>>>>>>>>>>>>>>>> that
>>>>>>>>>>>>>>>> are ψ-epistemic and those that are ψ-ontological are not 
>>>>>>>>>>>>>>>> decidable. There
>>>>>>>>>>>>>>>> is no decision procedure which can prove QM holds either way. 
>>>>>>>>>>>>>>>> The proof is
>>>>>>>>>>>>>>>> set with nonlocal hidden variables over the projective rays of 
>>>>>>>>>>>>>>>> the state
>>>>>>>>>>>>>>>> space. In effect there is an uncertainty in whether the hidden 
>>>>>>>>>>>>>>>> variables
>>>>>>>>>>>>>>>> localize extant quantities, say with ψ-ontology, or
>>>>>>>>>>>>>>>> whether this localization is the generation of information in 
>>>>>>>>>>>>>>>> a local
>>>>>>>>>>>>>>>> context from quantum nonlocality that is not extant, such as 
>>>>>>>>>>>>>>>> with
>>>>>>>>>>>>>>>> ψ-epistemology. Quantum interprertations are then
>>>>>>>>>>>>>>>> auxiliary physical axioms or postulates. MWI and within the 
>>>>>>>>>>>>>>>> framework of
>>>>>>>>>>>>>>>> what Carrol and Sebens has done this is a ψ-ontology, and
>>>>>>>>>>>>>>>> this defines the Born rule. If I am right the degree of 
>>>>>>>>>>>>>>>> ψ-epistemontic
>>>>>>>>>>>>>>>> nature is mixed. So the intriguing question we can address is 
>>>>>>>>>>>>>>>> the nature of
>>>>>>>>>>>>>>>> the Born rule and its tie into the auxiliary postulates of 
>>>>>>>>>>>>>>>> quantum
>>>>>>>>>>>>>>>> interpretations. Can a similar demonstration be made for the 
>>>>>>>>>>>>>>>> Born rule
>>>>>>>>>>>>>>>> within QuBism, which is what might be called the dialectic 
>>>>>>>>>>>>>>>> opposite of MWI?
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>> To take MWI as something literal, as opposed to maybe a
>>>>>>>>>>>>>>>> working system to understand QM foundations, is maybe taking 
>>>>>>>>>>>>>>>> things too
>>>>>>>>>>>>>>>> far. However, it is a part of some open questions concerning 
>>>>>>>>>>>>>>>> the
>>>>>>>>>>>>>>>> fundamentals of QM. If MWI, and more generally postulates
>>>>>>>>>>>>>>>> of quantum interpretations, are connected to the Born rule it 
>>>>>>>>>>>>>>>> makes for
>>>>>>>>>>>>>>>> some interesting things to think about.
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>> LC
>>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>> If you read the link, it's pretty obvious that Carroll
>>>>>>>>>>>>>>> believes the many worlds of the MWI, literally exist. AG
>>>>>>>>>>>>>>>
>>>>>>>>>>>>>>
>>>>>>>>>>>>>> Carroll also believes that IF the universe is infinite, then
>>>>>>>>>>>>>> there must exist exact copies of universes and ourselves. This is
>>>>>>>>>>>>>> frequently claimed by the MWI true believers, but never, AFAICT, 
>>>>>>>>>>>>>> proven, or
>>>>>>>>>>>>>> even plausibly argued.
>>>>>>>>>>>>>>
>>>>>>>>>>>>>>
>>>>>>>>>>>>>> The idea comes from Tegmark, and I agree with you, it
>>>>>>>>>>>>>> necessitate more than an infinite universe. It requires also some
>>>>>>>>>>>>>> assumption of homogeneity.
>>>>>>>>>>>>>>
>>>>>>>>>>>>>
>>>>>>>>>>>>> Our universe is, on a large scale, homogeneous. But it can't
>>>>>>>>>>>>> be infinite since it has only been expanding for finite time, 
>>>>>>>>>>>>> 13.8 BY. I
>>>>>>>>>>>>> had a discussion with Brent about this some time ago, and he 
>>>>>>>>>>>>> claimed finite
>>>>>>>>>>>>> in time doesn't preclude infinite in space. I strongly disagree. 
>>>>>>>>>>>>> Perhaps I
>>>>>>>>>>>>> am missing something. Wouldn't be the first time. AG
>>>>>>>>>>>>>
>>>>>>>>>>>>
>>>>>>>>>>>> I think what you may be missing is that in popular (but
>>>>>>>>>>>> misleading) accounts of the BB they often say everything 
>>>>>>>>>>>> originated from a
>>>>>>>>>>>> point, rather than everywhere at once.  To say "everything came 
>>>>>>>>>>>> from a
>>>>>>>>>>>> point" is at best only valid for describing the observable 
>>>>>>>>>>>> universe (or any
>>>>>>>>>>>> finite portion of the universe) but is invalid to extrapolate it 
>>>>>>>>>>>> to the
>>>>>>>>>>>> whole universe, which may be spatially infinite.
>>>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>> I am not assuming our universe began from a mathematical point,
>>>>>>>>>>> but I do assume that 13.8 BYA it was very very small, the 
>>>>>>>>>>> observable and
>>>>>>>>>>> unobservable parts.
>>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>> Why do you assume this?  Most cosmologists make no such
>>>>>>>>>> assumption.  Under the concordance (standard assumed) model of 
>>>>>>>>>> cosmology,
>>>>>>>>>> space is infinite.
>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>>  I don't think there is an implied disconnect between our
>>>>>>>>>>> measurements of the CMBR and what an observer would measure in 
>>>>>>>>>>> parts we
>>>>>>>>>>> have no access to. It was everywhere hot and dense, and very very 
>>>>>>>>>>> small.
>>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>> There's no observational motivation for the universe being very
>>>>>>>>>> very small at the beginning.  It could have been small, large or 
>>>>>>>>>> infinite,
>>>>>>>>>> for all we know.
>>>>>>>>>>
>>>>>>>>>
>>>>>>>>> I've never read a description of inflation where the universe is
>>>>>>>>> described as very large spatially when it initiates. Never. It's 
>>>>>>>>> always
>>>>>>>>> claimed it begins a few Planck durations (10^-43 seconds) after the 
>>>>>>>>> BB, at
>>>>>>>>> which time the spatial diameter is many orders of magnitudes smaller 
>>>>>>>>> than
>>>>>>>>> the diameter of a proton. It then expands to the diameter of the 
>>>>>>>>> Earth or
>>>>>>>>> the Solar System before terminating, all this occuring within the 
>>>>>>>>> first
>>>>>>>>> second after the BB. AG
>>>>>>>>>
>>>>>>>>
>>>>>>>> I think we need to clearly distinguish between three periods, which
>>>>>>>> are frequently confused:
>>>>>>>>
>>>>>>>> 1. "quantum vacuum phase" Size: ??? Time: ???
>>>>>>>> If inflation began as a fluctuation in the vacuum, the vacuum was a
>>>>>>>> pre-existing initial condition. We can say nothing of it's size or how 
>>>>>>>> long
>>>>>>>> it has existed.  Alternatively, this vacuum may have already been in a
>>>>>>>> state of exponential expansion and required no fluctuation to get 
>>>>>>>> started.
>>>>>>>>
>>>>>>>>
>>>>>>>> 2. "Inflation start" Size: (min = Planck size, max = ???) Time:
>>>>>>>> (min = fraction of second before hot stage of BB, max = finite but
>>>>>>>> otherwise unlimited time ago).
>>>>>>>> If inflation started as a fluctuation it could have started very
>>>>>>>> small, but it would then grow exponentially forever.  How big it was 
>>>>>>>> when
>>>>>>>> it stopped for us we can't say, but we can guess it had to have gone 
>>>>>>>> on for
>>>>>>>> at least 10^-32 seconds to fit with observations.  This is only the 
>>>>>>>> minimum
>>>>>>>> time, there's no known upper bound.  There's not necessarily any 
>>>>>>>> cooling
>>>>>>>> during this time as the heat doesn't enter the picture until inflation
>>>>>>>> begins to stop somewhere.
>>>>>>>>
>>>>>>>> 3. "Local inflation end", Size of inflating space: (undefined but
>>>>>>>> ever growing), Size of pocket from outside: (finite but growing), 
>>>>>>>> Apparent
>>>>>>>> size of pocket from inside: (finite or infinite depending on shape of 
>>>>>>>> the
>>>>>>>> universe), Time: 13.8 BY ago.
>>>>>>>>
>>>>>>>> The "T = 0 of the BB" no longer makes sense in the inflation
>>>>>>>> picture, the only place we can begin to speak of absolutes with time is
>>>>>>>> when we speak of the local end to inflation in our pocket.
>>>>>>>>
>>>>>>>> Jason
>>>>>>>>
>>>>>>>
>>>>>>> I'll say it again. One the main reasons to posit inflation is to
>>>>>>> explain the observable large scale homogeneity of a universe that is now
>>>>>>> NOT causally connected. If the universe was very very tiny when 
>>>>>>> inflation
>>>>>>> started, it WAS then causally connected,
>>>>>>>
>>>>>>
>>>>>> The *observable* part of the universe is posited to have once been
>>>>>> causally connected to come to thermal equilibrium but not necessarily the
>>>>>> entire universe.
>>>>>>
>>>>>
>>>>> OK, but based on our best measurements, we live in a closed,
>>>>> accelerating and expanding hypersphere, since the curvature is NOT zero 
>>>>> and
>>>>> NOT negative.
>>>>>
>>>>
>>>> Do you have a citation for this?  All the estimates I am familiar with
>>>> assume a flat or slightly open shape.
>>>>
>>>>
>>>>> I prefer to go with what we think we know, rather than with a model
>>>>> which is completely speculative. AG
>>>>>
>>>>
>>>> Which is what?
>>>>
>>>
>>> I am looking for a citation, but I recall that someone on this thread
>>> stated the measured curvature is close to zero, but POSITIVE. AG
>>>
>>
>> Okay.
>>
>>
>>>
>>>>
>>>>>
>>>>>>
>>>>>>> and inflation preserved the homogeneity. This is what Guth was
>>>>>>> trying to solve with inflation, among other problems, such as no 
>>>>>>> detectable
>>>>>>> monopoles. This entire logic breaks down if one assumes an infinite
>>>>>>> universe at the time of inflation.
>>>>>>>
>>>>>>
>>>>>> Correct, using inflation and previous causal connectedness does not
>>>>>> produce for homogeneity of temperature to all parts of the universe if 
>>>>>> the
>>>>>> universe is infinite.
>>>>>>
>>>>>
>>>>> So far, as I just stated, our best evidence
>>>>>
>>>>
>>>> There's no evidence either way, as far as I am aware, which is why i is
>>>> still considered an open question.  If you can point me to some evidence I
>>>> would be interested.
>>>>
>>>>
>>>>> does NOT suggest an infinite universe. AG
>>>>>
>>>>
>>>> What are you calling as the universe here?  How are you defining it?
>>>>
>>>
>>> I am referring to our bubble, which arose with the BB, and refers to the
>>> observable and UNobservable regions (not to the possibly infinite substrate
>>> from which it arose). AG
>>>
>>
>> Alright.  Then you also need to clarify which perspective you are using.
>> Since the bubble may be finite from the outside, but can appear infinite
>> from the inside.
>>
>
> Since there's no way to observe the bubble from the outside, I don't see
> this as productive way to analyse the situation. AG
>
>>
>>
>>>
>>>>
>>>>>
>>>>>
>>>>>>   At best it can only extend to some finite region of that universe.
>>>>>> But once you are working in an inflationary model, you already have
>>>>>> accepted there is a large scale where the universe is not homogenous
>>>>>> (pocket regions vs. the rapidly inflating regions of vacuum).
>>>>>>
>>>>>
>>>>> I don't see why assuming inflation implies acceptance of large parts
>>>>> of the UNobservable universe which is NOT homogeneous. AG
>>>>>
>>>>
>>>> Because decay events of the vacuum do not happen everywhere at once,
>>>> this leads to isolated "pocket universes" separated by exponentially
>>>> expanding space.  The inhomogenity I am referring to are the different
>>>> parts of the vacuum in different energy states.
>>>>
>>>>
>>>>>
>>>>>>
>>>>>>> In this case, the infinite universe was always homogeneous even
>>>>>>> though it was never causally connected.
>>>>>>>
>>>>>>
>>>>>> That is another possibility that avoids inflation as an explanation
>>>>>> of homogeneity:  To simply assume everything at all places began at the
>>>>>> same temperature and density.
>>>>>>
>>>>>
>>>>> If so, why did Guth think homogeneity needed an explanation? On its
>>>>> face, thermal equilibrium for a non causally connected universe seems
>>>>> improbable. AG
>>>>>
>>>>
>>>> It came for free, with the other explanations.  On its own, I am not
>>>> sure it would be justified to trade one assumption for another, but
>>>> inflation replaced 4 or 5 assumptions with a single one, which is its main
>>>> strength.
>>>>
>>>>
>>>>>
>>>>>>
>>>>>>> Further, how could it have been so hot 380,000 years after the BB if
>>>>>>> it wasn't dense at that time?
>>>>>>>
>>>>>>
>>>>>> Actually the universe was not very dense at the time of 380,000
>>>>>> years.  It was billions of times more sparse than Earth's atmosphere.  
>>>>>> Each
>>>>>> time the scale factor
>>>>>> <https://en.wikipedia.org/wiki/Scale_factor_(cosmology)> halves
>>>>>> going backwards in time, the temperature doubles, and the density 
>>>>>> increases
>>>>>> by a factor of 8 (2 cubed).  You can follows this backwards at least 
>>>>>> until
>>>>>> the temperature is about 10^27 K, far far hotter and denser than 380,000
>>>>>> years, back to a time just a fraction of a second after inflation ended.
>>>>>>
>>>>>
>>>>> Yes, it was far hotter and denser just after the BB, than at 380,000
>>>>> years.
>>>>>
>>>>
>>>> Okay.
>>>>
>>>>
>>>>> But contrary to what you allege above and below, it must have far
>>>>> hotter and denser at 380,000 years, than it is today, 2.7 deg K, so hot 
>>>>> and
>>>>> dense that it was opaque to light.
>>>>>
>>>>
>>>> I'm not sure how this is contrary to what I say above and below...  I
>>>> agree it was hotter and denser the farther back you go.
>>>>
>>>
>>> And smaller as well? (BTW, "smaller" can't be a property of a spatially
>>> infinite universe.)
>>>
>>
>> Smaller is not implied by the big bang model, only things being
>> "previously closer".
>>
>
> True, but if *inflation* is to solve the large scale homogeneity property
> of our present universe, which it does, inflation had to occur when the
> universe was exceedingly small. See my previous post on this issue. AG
>

I would make this correction:
> True, but if inflation is to solve the large scale homogeneity property
of our present universe, which it does, inflation had to occur when the
*OBSERVABLE* universe was exceedingly small. See my previous post on this
issue. AG


>
>
>> I know many popular accounts of the BB say the universe was once smaller,
>> but this is sloppy writing.  They are referring to some fixed part of the
>> universe being smaller, such as the observable part.  But to say the
>> universe in total was smaller is to assume one knows if it is infinite or
>> finite, open/flat or closed.  This is not known, so no accurate account of
>> the BB would implicitly assume it to be known.
>>
>>
>>> It had to have gotten smaller to explain its present homogeneity. I want
>>> to avoid the assumption that homogeneity can arise spontaneously in a
>>> causally DIS-connected universe, the one we observe.
>>>
>>
>> But to explain that rather than assuming it, then you need inflation, but
>> below you call this "totally speculative".  Which is it?
>>
>>
>>> And I don't believe that at 380,000 years it was less dense than our
>>> atmosphere (as you earlier alleged). AG
>>>
>>
>> The present density of the universe is about 5 hydrogen atoms per cubic
>> meter.  At the time of 380,000 years, things were ~1100x closer together
>> (the scale factor is ~1/1100) compared to today.  This is a simple
>> calculation of the temperature difference. If it's 2.73K now, and it was
>> 3000K then, then the scale factor growth from then to now is 3000/2.73 =
>> 1098.
>>
>> If each dimension changed by a factor of 1,000, this means the density
>> back then would have been 1,000 x 1,000 x 1,000 or a billion times what it
>> is now.  So instead of 5 hydrogen atoms per cubic meter, you get 5 billion
>> hydrogen atoms per cubic meter.  This is many many orders of magnitude less
>> dense than atmospheric pressure.  A cubic meter of air at sea level weighs
>> 1.3 kilograms ( https://hypertextbook.com/facts/2000/RachelChu.shtml ).
>> Compare this weight to the weight of 5 billion hydrogen atoms.  A Hydogen
>> atom weighs 1.67 × 10^-24 g, 5 billion of them would get you to 8.37 ×
>> 10^-18 kilograms.
>>
>> So I was wrong, it wasn't a billion times less dense, it was closer to a
>> billion billion times less dense than the atmosphere.
>>
>>
>>>
>>>>
>>>>> I am just saying that it does seem to be cooling as it expands,
>>>>>
>>>>
>>>> Yes.
>>>>
>>>>
>>>>> and the curvature data seems to imply smallness just after the BB.
>>>>>
>>>>
>>>> What curvature data are you referring to?  The latest Planck data say
>>>> the curvature is flat to within the limits of our measurement accuracy.  Is
>>>> there a new result that indicates positive curvature?
>>>>
>>>
>>> "Flat" means curvature is exactly zero; that is, flat like a Euclidean
>>> plane. But if we measure slightly positive, which I think is the case, it
>>> must be a closed hyperspace, but HUGE. Physicists tend to equate "almost
>>> flat", which if true would mean a huge spherical hyperspace, with Euclidean
>>> flat. This is a persistent error. AG
>>>
>>> What I don't understand is why, a universe with accelerating expansion,
>>> must be open, like a saddle.
>>>
>>
>> The shape (closed, flat, open), depends on how much gravitating stuff is
>> in the universe compared to how much anti-gravitating stuff is in the
>> universe, and the current expansion rate and density.  A closed universe
>> implies gravitational attraction wins out in the end and things eventually
>> collapse.  In a universe where there is more gravitating stuff then anti
>> gravitating stuff, the speed of expansion ought to be slowing down.  If it
>> is slowing down in a way that only after infinite time the expansion rate =
>> 0 (loosely analogous to throwing something upwards at exactly the escape
>> velocity) then the geometry is flat.  But the only way for the universe
>> expansion to be accelerating now is if the anti-gravity stuff exceeds the
>> gravitating stuff.  In this case, (should the condition persist), then the
>> universe will not recollapse (can't be closed), nor will it come to a rest
>> after infinite time (can't be flat), so the alternative is that it must be
>> open.
>>
>
> That's what the books say. But suppose the universe was a spherical
> expanding hyperspace at some point in its history, closed, and then the
> expansion rate started to increase. Would that closed universe somehow
> "tear" and become open? AG
>

I'm not sure, it is a good question if the shape can evolve over time.
Perhaps someone on this list more familiar with GR can answer.


>
>>
>>> Why can't a spherical hyperspace retain its closure if its expansion is
>>> accelerating? AG
>>>
>>
>> Mathematically you can of course imagine an ever expanding hypersphere,
>> but the reason it is not possible physically is comes down to general
>> relativity, which informs of us of a relationship between the spatial
>> curvature and the ultimate fate of the universe.  So if anti-gravity stuff
>> wins out such that the universe expands forever in an accelerating or
>> constant rate, then GR requires that the spatial curvature be negative.  It
>> would not allow for a positive curvature.
>>
>
> I find this rather dubious. Can you show me how GR requires this? AG
>

It is made clear in the Friedmann equations, which are derived from the
field equations of GR:
https://en.wikipedia.org/wiki/Friedmann_equations
Where they contain a parameter k which is either -1, 0, or 1, corresponding
to the curvature of space.  The value of k determines how the expansion
rate changes over time.

Jason


>
>>
>>>
>>>>
>>>>> Moreover, applying the Cosmological principle, it couldn't have been
>>>>> homogeneous on large scale in the finite observable region, and at the 
>>>>> same
>>>>> time infinite and non-homogeneous in regions we can't observe. AG
>>>>>
>>>>
>>>> It all comes down to scale.  At the scale of stars or galaxies, the
>>>> universe is non homogeneous, on the scale of super clusters and above it
>>>> is, but at larger scales of inflating vacuums and pocket universes, again
>>>> it is non homogeneous, but perhaps if you zoom out far enough the picture
>>>> becomes homogeneous again.  The non-homogeneous part I am referring to can
>>>> be seen as the spiky image, a rendering of eternal inflation:
>>>> https://www.preposterousuniverse.com/blog/2011/10/21/the-eternally-existing-self-reproducing-frequently-puzzling-inflationary-universe/
>>>>
>>>
>>> I would forget about inflating vacuums and pocket universes, which are
>>> totally speculative,
>>>
>>
>> They're more or less a direct consequence of inflation.  Inflation is a
>> little bit more than totally speculative.  I would go so far to saying it
>> is at least weakly confirmed.
>>
>>
>>> and focus on what we can observe -- which, on a large scale, is
>>> homogeneous. Why trash the Cosmological Principle by appealig to
>>> unobservable phenomena? AG
>>>
>>
>> The cosmological principle is not a firm rule or law, it is a rule of
>> thumb which works under the assumption that the same laws operate
>> everywhere and same conditions hold everywhere, and therefore things should
>> be roughly the same everywhere.  Inflation tells us that at certain scales
>> the conditions are not the same everywhere, so we should not expect
>> everything to seem homogeneous at those scales.
>>
>
> The same laws must operate everywhere; otherwise we can't do physics. But
> obviously, within those laws, whatever they are, different events can occur
> in different locations. AG
>
>>
>> Jason
>>
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