On 21-Dec-2019, at 6:33 AM, Alan Grayson <agrays...@gmail.com> wrote:
I've argued for this several times based on logic, not data, and as far as I can recall, no one took me seriously. AGhttps://thenextweb.com/syndication/2019/12/17/cosmology-in-crisis-as-evidence-suggests-our-universe-isnt-flat-its-actually-curved/
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I've argued for this several times based on logic, not data, and as far as I can recall, no one took me seriously. AGhttps://thenextweb.com/syndication/2019/12/17/cosmology-in-crisis-as-evidence-suggests-our-universe-isnt-flat-its-actually-curved/
(a'/a)^2 = (8piG/3c^2) - k/a^2,
for k = 0 being flat space, k = 1 for a sphere and k = -1 for a hyperboloid. As a, the scale factor becomes large the last term is small.
The bias for flatness comes from inflation, where a region of an inflationary spacetime with large vacuum energy tunnels into a small vacuum energy. This results in so called pocket world's. There is a boundary to the high energy region. By the Gauss-Bonnett theorem this boundary has information. A type of quantum phase change may change the topology into a sphere that "pops off" the inflationary manifold. So for me this might be welcome news if the observable cosmos is spherical.
Inflation involves the vacuum transition to a small value in a bounded region in the de Sitter manifold of inflation. Hence flatness. If there observable universe is an expanding 3-sphere there is more to this than current phenomenology.
LC
Your objection to flatness is wrong. During inflation the cosmic horizon scale was a million billion times smaller than a proton. That transitioned into the large scale of today. This can still happen in a flat infinite spacetime.
LC
It is not about a small volume becoming infinite. It is about mass-energy density becoming lower.
LC
LC
Sigh! Mass-energy is extensive through out. It's density keeps lowering as particles are frame dragged.LC
LC
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On 22 Dec 2019, at 02:35, Alan Grayson <agrays...@gmail.com> wrote:
On Saturday, December 21, 2019 at 5:52:28 PM UTC-7, Lawrence Crowell wrote:Sigh! Mass-energy is extensive through out. It's density keeps lowering as particles are frame dragged.LC
I don't dispute your point (though I don't see the role of frame dragging). But can you answer a simple question? Are flat and saddle-shaped universes spatially infinite or not? TIA, AGI tend to make sense of your question, in the case we agree that space itself is born with the big-bang (which I am quite not sure), it is hard to imagine it could be infinite in size at any fine moment I guess Lawrence assume some space before the Big Bang, if that make sense. I think we need to solve the problem of quantum gravitation, that is a quantum theory of space-time, to handle this question. (I am not an expert on this to be sure).Bruno
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If the observable universe is curved as a sphere it means this bubble "popped off" the inflationary manifold. This throws new unknowns into the matter.
I am not it was not infinite. The big bang is due, within the inflationary phenomenology, to a region of the inflationary de Sitter space being an unstable vacuum that transitioned to a lower energy. The energy density gap produced particles and radiation. So the observable universe is a bubble in the "Swiss cheese." The dS spacetime is infinite in extent.
If the observable universe is curved as a sphere it means this bubble "popped off" the inflationary manifold. This throws new unknowns into the matter.
LC
Look up inflationary cosmology or eternal inflation. Wikipedia has a page on this.LC
LC
These bubbles are not spheres, but rather balls with a boundary. The boundary contains QFT data for fields in the inflationary spacetime. If this bubble "pops off" the inflationary spacetime that boundary information defines the topology, or topological quantum numbers, for this disconnected 3-sphere.LC
LC
Inflation is on the dS that is spatially flat. A bubble with broken vacuum symmetry is also flat. If the observable cosmos is not flat this upsets some apple carts.LC
LC
LC
Velinkin has shown that eternal inflating dS or dS-like spaces are not eternal in the past. They are so into the future. What comes "before," if that makes sense, is not known. The problem is that any extension of time here into that domain, say by translation of coordinates, is questionable.
LC
LC
LC
Sure there are! The main phenom for the cosmos is spatially flat and infinite. Red shift and horizons mean any observer can only access a finite amount of information.LC
Sure there are! The main phenom for the cosmos is spatially flat and infinite. Red shift and horizons mean any observer can only access a finite amount of information.LC
In either case, finite or infinite, one is confronted with some unpleasant realities. If the universe is strictly finite there is always an uncomfortable sense that a finite set is bounded, and as such there can potentially be something outside it. If the universe is infinite then how can we completely understand it?
LC
LC
Not quite. There are subtle differences that at least in principle are observable.LC
Not quite. There are subtle differences that at least in principle are observable.LC
I've argued for this several times based on logic, not data, and as far as I can recall, no one took me seriously. AGhttps://thenextweb.com/syndication/2019/12/17/cosmology-in-crisis-as-evidence-suggests-our-universe-isnt-flat-its-actually-curved/
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@philipthrift
LC
On Saturday, December 21, 2019 at 4:42:50 AM UTC-7, Lawrence Crowell wrote:If the observable universe is a closed sphere that might be a boost for me. The FLRW constraint is(a'/a)^2 = (8piG/3c^2) - k/a^2,
for k = 0 being flat space, k = 1 for a sphere and k = -1 for a hyperboloid. As a, the scale factor becomes large the last term is small.
The bias for flatness comes from inflation, where a region of an inflationary spacetime with large vacuum energy tunnels into a small vacuum energy. This results in so called pocket world's. There is a boundary to the high energy region. By the Gauss-Bonnett theorem this boundary has information. A type of quantum phase change may change the topology into a sphere that "pops off" the inflationary manifold. So for me this might be welcome news if the observable cosmos is spherical.
I argued two or three times with Brent and others, that the curvature cannot be exactly zero, or negative -- corresponding to flat or saddle-shaped universes -- because both are infinite in spatial extent, which contradicts the models of the cosmos being extremely tiny near the BB. They also contradict the concept of the cosmos expanding for finite time, at less than infinite speed. So it seemed clear, that the cosmos must be spherical in shape, with a positive curvature, very close to zero, but not zero -- which is what is measured. I don't see why my arguments made no impact. Now I don't understand why a spherical universe somehow poses a problem for inflation, which still seems needed to explain the large scale homogeneity. AG
There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3
On Monday, January 6, 2020 at 2:18:48 PM UTC-7, Pierz wrote:There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3TY. I viewed this. It explains nothing. What he calls "the infinite flat sheet" at the initiation of the BB is not "our universe". Rather, what I call "our universe" is the observable and unobservable regions, where the latter is created as a result of faster-than-light inflation. Toth's infinite flat sheet is what I have referred to as the substratum from which our universe emerged. It could be flat, or even saddle-shaped, but it is not our universe with two regions as just defined. AG
On Monday, January 6, 2020 at 2:18:48 PM UTC-7, Pierz wrote:There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3
TY. I viewed this. It explains nothing. What he calls "the infinite flat sheet" at the initiation of the BB is not "our universe". Rather, what I call "our universe" is the observable and unobservable regions, where the latter is created as a result of faster-than-light inflation. Toth's infinite flat sheet is what I have referred to as the substratum from which our universe emerged. It could be flat, or even saddle-shaped, but it is not our universe with two regions as just defined. AG
On 1/6/2020 2:00 PM, Alan Grayson wrote:
On Monday, January 6, 2020 at 2:18:48 PM UTC-7, Pierz wrote:There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3
TY. I viewed this. It explains nothing. What he calls "the infinite flat sheet" at the initiation of the BB is not "our universe". Rather, what I call "our universe" is the observable and unobservable regions, where the latter is created as a result of faster-than-light inflation. Toth's infinite flat sheet is what I have referred to as the substratum from which our universe emerged. It could be flat, or even saddle-shaped, but it is not our universe with two regions as just defined. AG
You can call it whatever you want, but it's what is described by the FLRW solution of Einstein's equations for the cosmos. What part is observable is relative to us.
Brent
On Monday, January 6, 2020 at 3:50:55 PM UTC-7, Brent wrote:
On 1/6/2020 2:00 PM, Alan Grayson wrote:
On Monday, January 6, 2020 at 2:18:48 PM UTC-7, Pierz wrote:There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3
TY. I viewed this. It explains nothing. What he calls "the infinite flat sheet" at the initiation of the BB is not "our universe". Rather, what I call "our universe" is the observable and unobservable regions, where the latter is created as a result of faster-than-light inflation. Toth's infinite flat sheet is what I have referred to as the substratum from which our universe emerged. It could be flat, or even saddle-shaped, but it is not our universe with two regions as just defined. AG
You can call it whatever you want, but it's what is described by the FLRW solution of Einstein's equations for the cosmos. What part is observable is relative to us.
Brent
I looked up the FLRW solution on Wiki. https://en.wikipedia.org/wiki/Friedmann%E2%80%93Lema%C3%AEtre%E2%80%93Robertson%E2%80%93Walker_metric#Curvature
I see there's a parameter k which determines curvature, but the mathematics doesn't seem to give what the value is, other than three possibilities; -1 ,0, 1.
If this is true, how can the solution you suggest shed any light on what the actually curvature is? Moreover, I would think measured values would trump hypothetical possibilities, and the article which I posted starting this discussion alleges that the measured value, although falling short of 5-sigma certainty, indicates a spherical shape. TIA, AG
On Sunday, December 22, 2019 at 7:37:25 AM UTC+11, Alan Grayson wrote:
On Saturday, December 21, 2019 at 4:42:50 AM UTC-7, Lawrence Crowell wrote:If the observable universe is a closed sphere that might be a boost for me. The FLRW constraint is(a'/a)^2 = (8piG/3c^2) - k/a^2,
for k = 0 being flat space, k = 1 for a sphere and k = -1 for a hyperboloid. As a, the scale factor becomes large the last term is small.
The bias for flatness comes from inflation, where a region of an inflationary spacetime with large vacuum energy tunnels into a small vacuum energy. This results in so called pocket world's. There is a boundary to the high energy region. By the Gauss-Bonnett theorem this boundary has information. A type of quantum phase change may change the topology into a sphere that "pops off" the inflationary manifold. So for me this might be welcome news if the observable cosmos is spherical.
I argued two or three times with Brent and others, that the curvature cannot be exactly zero, or negative -- corresponding to flat or saddle-shaped universes -- because both are infinite in spatial extent, which contradicts the models of the cosmos being extremely tiny near the BB. They also contradict the concept of the cosmos expanding for finite time, at less than infinite speed. So it seemed clear, that the cosmos must be spherical in shape, with a positive curvature, very close to zero, but not zero -- which is what is measured. I don't see why my arguments made no impact. Now I don't understand why a spherical universe somehow poses a problem for inflation, which still seems needed to explain the large scale homogeneity. AG
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On 1/6/2020 9:15 PM, Alan Grayson wrote:
On Monday, January 6, 2020 at 3:50:55 PM UTC-7, Brent wrote:
On 1/6/2020 2:00 PM, Alan Grayson wrote:
On Monday, January 6, 2020 at 2:18:48 PM UTC-7, Pierz wrote:There are sooo many examples of this misconception on Quora. Here's one answer from Viktor Toth, who is excellent with the late explanations: https://qr.ae/TSjfO3
TY. I viewed this. It explains nothing. What he calls "the infinite flat sheet" at the initiation of the BB is not "our universe". Rather, what I call "our universe" is the observable and unobservable regions, where the latter is created as a result of faster-than-light inflation. Toth's infinite flat sheet is what I have referred to as the substratum from which our universe emerged. It could be flat, or even saddle-shaped, but it is not our universe with two regions as just defined. AG
You can call it whatever you want, but it's what is described by the FLRW solution of Einstein's equations for the cosmos. What part is observable is relative to us.
Brent
I looked up the FLRW solution on Wiki. https://en.wikipedia.org/wiki/Friedmann%E2%80%93Lema%C3%AEtre%E2%80%93Robertson%E2%80%93Walker_metric#Curvature
I see there's a parameter k which determines curvature, but the mathematics doesn't seem to give what the value is, other than three possibilities; -1 ,0, 1.
That's because the specific value of curvature can be absorbed into the initial conditions, so only the sign of k matters.
If this is true, how can the solution you suggest shed any light on what the actually curvature is? Moreover, I would think measured values would trump hypothetical possibilities, and the article which I posted starting this discussion alleges that the measured value, although falling short of 5-sigma certainty, indicates a spherical shape. TIA, AG
The FLRW solution assumes isotropy and homogeneity which together imply spherical symmetry. But that's probably not what you mean by "shape".
Brent
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On Sunday, December 22, 2019 at 7:37:25 AM UTC+11, Alan Grayson wrote:
On Saturday, December 21, 2019 at 4:42:50 AM UTC-7, Lawrence Crowell wrote:If the observable universe is a closed sphere that might be a boost for me. The FLRW constraint is(a'/a)^2 = (8piG/3c^2) - k/a^2,
for k = 0 being flat space, k = 1 for a sphere and k = -1 for a hyperboloid. As a, the scale factor becomes large the last term is small.
The bias for flatness comes from inflation, where a region of an inflationary spacetime with large vacuum energy tunnels into a small vacuum energy. This results in so called pocket world's. There is a boundary to the high energy region. By the Gauss-Bonnett theorem this boundary has information. A type of quantum phase change may change the topology into a sphere that "pops off" the inflationary manifold. So for me this might be welcome news if the observable cosmos is spherical.
I argued two or three times with Brent and others, that the curvature cannot be exactly zero, or negative -- corresponding to flat or saddle-shaped universes -- because both are infinite in spatial extent, which contradicts the models of the cosmos being extremely tiny near the BB. They also contradict the concept of the cosmos expanding for finite time, at less than infinite speed. So it seemed clear, that the cosmos must be spherical in shape, with a positive curvature, very close to zero, but not zero -- which is what is measured. I don't see why my arguments made no impact. Now I don't understand why a spherical universe somehow poses a problem for inflation, which still seems needed to explain the large scale homogeneity. AG
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Gödel's cosmology violates the Hawking-Penrose condition T^{00} >= 0. This corresponds to the closed timelike curves in the spacetimes. The whole cosmology has a net angular momentum that frame drags geodesics into closed timelike curves.
LC
LC
Energy is positive.LC
LC
Energy is positive.LC
LC
The T^{00} >= 0, which is the vev, or defines H, but the gravitational potential is negative. The sum is zero.LC
The Hamiltonian H = ½(a’)^2 - 4πGρ/3c^2 is zero. Here a is the scale factor a' the time derivative and ρ the vacuum energy density. By positive it means that ρ is;positive and the kinetic energy ½(a’)^2 is positive. The gravitational potential energy - 4πGρ/3c^2 is negative.LC.
On Friday, January 10, 2020 at 6:52:47 PM UTC-7, Lawrence Crowell wrote:The Hamiltonian H = ½(a’)^2 - 4πGρ/3c^2 is zero. Here a is the scale factor a' the time derivative and ρ the vacuum energy density. By positive it means that ρ is;positive and the kinetic energy ½(a’)^2 is positive. The gravitational potential energy - 4πGρ/3c^2 is negative.LC.Is gravitational potential energy well defined in Newtonian physics? I think not, for the reasons previously given. AG
On Saturday, January 11, 2020 at 2:17:32 AM UTC-6, Alan Grayson wrote:
On Friday, January 10, 2020 at 6:52:47 PM UTC-7, Lawrence Crowell wrote:The Hamiltonian H = ½(a’)^2 - 4πGρ/3c^2 is zero. Here a is the scale factor a' the time derivative and ρ the vacuum energy density. By positive it means that ρ is;positive and the kinetic energy ½(a’)^2 is positive. The gravitational potential energy - 4πGρ/3c^2 is negative.LC.Is gravitational potential energy well defined in Newtonian physics? I think not, for the reasons previously given. AGIt is well defined. The FLRW and de Sitter spacetimes on the Hubble frame reduce to a Newtonian description, for the most part except the term -k/a^2. This works well enough.LC
On Saturday, January 11, 2020 at 3:10:40 AM UTC-7, Lawrence Crowell wrote:On Saturday, January 11, 2020 at 2:17:32 AM UTC-6, Alan Grayson wrote:
On Friday, January 10, 2020 at 6:52:47 PM UTC-7, Lawrence Crowell wrote:The Hamiltonian H = ½(a’)^2 - 4πGρ/3c^2 is zero. Here a is the scale factor a' the time derivative and ρ the vacuum energy density. By positive it means that ρ is;positive and the kinetic energy ½(a’)^2 is positive. The gravitational potential energy - 4πGρ/3c^2 is negative.LC.Is gravitational potential energy well defined in Newtonian physics? I think not, for the reasons previously given. AGIt is well defined. The FLRW and de Sitter spacetimes on the Hubble frame reduce to a Newtonian description, for the most part except the term -k/a^2. This works well enough.LCIf you Int (Fdr) from some r to infinity, you get the potential energy at r, but it blows up as you get to the center of mass. For me, this indicates the PE in Newtonian gravity is not well defined. No? AG
On Saturday, January 11, 2020 at 5:37:02 AM UTC-6, Alan Grayson wrote:
On Saturday, January 11, 2020 at 3:10:40 AM UTC-7, Lawrence Crowell wrote:On Saturday, January 11, 2020 at 2:17:32 AM UTC-6, Alan Grayson wrote:
On Friday, January 10, 2020 at 6:52:47 PM UTC-7, Lawrence Crowell wrote:The Hamiltonian H = ½(a’)^2 - 4πGρ/3c^2 is zero. Here a is the scale factor a' the time derivative and ρ the vacuum energy density. By positive it means that ρ is;positive and the kinetic energy ½(a’)^2 is positive. The gravitational potential energy - 4πGρ/3c^2 is negative.LC.Is gravitational potential energy well defined in Newtonian physics? I think not, for the reasons previously given. AGIt is well defined. The FLRW and de Sitter spacetimes on the Hubble frame reduce to a Newtonian description, for the most part except the term -k/a^2. This works well enough.LCIf you Int (Fdr) from some r to infinity, you get the potential energy at r, but it blows up as you get to the center of mass. For me, this indicates the PE in Newtonian gravity is not well defined. No? AGThat is no more of a problem than r = 0. For finite differences it works fine.LC
If you Int (Fdr) from some r to infinity, you get the potential energy at r, but it blows up as you get to the center of mass. For me, this indicates the PE in Newtonian gravity is not well defined. No? AG
Brent
Brent
I've argued for this several times based on logic, not data, and as far as I can recall, no one took me seriously. AGhttps://thenextweb.com/syndication/2019/12/17/cosmology-in-crisis-as-evidence-suggests-our-universe-isnt-flat-its-actually-curved/