On the general curvature of space.

In summary, cosmologists generally accept that the universe is flat, meaning that it has a C value of 0. This is supported by basic geometric principles such as parallel lines not intersecting and the angles of a triangle adding up to 180 degrees. The equation used to describe this curvature is the Friedmann Equation, which takes into account factors such as density of matter, the cosmological constant, and Hubble's constant. While some theorize about the possibility of a curved universe, there is no evidence to support this and it goes against established principles. The question of the universe's expansion is a separate issue, with theories suggesting either an open, balanced, or closed universe. However, the concept of the vacuum having density raises questions about gravitational
  • #1
quasar987
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What is actually commonly accepted in the cosmologist society regarding the model of the universe? Do they think C=0 or > 0 or < 0 ? And what makes them think that?


Also, how do one get the shapes related to each posibility for C from the equations of GR?
 
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  • #2
I'm not sure I understand your question. People think (actually they know) that c= 3.00 x 10^8 m/s.
 
  • #4
I should have specified that I had the following equation in mind while writing the question...

[itex] C=k(\rho + \Lambda) - H^2 [/itex]

Where [itex] C [/itex] is the overall curve of space (C = 0 meaning a flat universe, C > 0 meaning a closed universe and a C < 0 meaning a universe shaped like a sadle),
[itex] k [/itex] is a constant meant to make the dimensions from the right hand side of the equation match the dimensions of the left hand side.
[itex] \rho [/itex] is the density of matter
[itex] \Lambda [/itex] is the cosmological constant (or density of the vacuum)
[itex] H [/itex] is Hubble's constant.
 
  • #5
We all know that the universe is flat, because of basic reasons. For example, parallel lines don't intersect, the angles of a triangle add up to 180 degerees, ect. If we lived in a curved universe, none of this would be true.
 
  • #6
We all know that the universe is flat, because of basic reasons. For example, parallel lines don't intersect, the angles of a triangle add up to 180 degerees, ect. If we lived in a curved universe, none of this would be true.

We know that those facts are true locally. They might not hold up if you examine a larger region of the universe.
 
  • #7
I think there are two different problems trying to be solved by one theory that doesn’t apply to either.

The first question is the physical curve of the universe.

If the universe started out from the Big Bang then it expanded in all directions and forms and has always formed a sphere, or a curved surface.

This is a three dimensional hypersphere. If you examine the universe from this point of view you must come to the conclusion that the universe is a geometrical curve.

The second question is the nature or the forces of the expansion.
This is where the concept of open, balanced, or closed universe comes into play.

Not going into my personal theory, there is no explanation for the expansion except the result of an initial explosion and the law of inertia.

The law of inertia states that bodies in motion continue in motion unless acted on by a force.

With out a slowing force the universe would expand at the same rate forever. This is the open universe.

If the force of gravity is able to act on the expanding universe then the question is, will it slow the universe expansion and create a closed universe.
 
  • #8
4Newton said:
If the force of gravity is able to act on the expanding universe then the question is, will it slow the universe expansion and create a closed universe.
In the book I took the formula from, they say it can be shows that if, at any time, the universe had a positive/negative/zero C, then it has always been so and will always be. In other words, the universe CANNOT change from open to flat to closed.

Another thing that's bugging me is, if the vacuum has density, then it should be subject to gravitationnal attraction, shouldn't it? I never heard anyone mention that though.
 
  • #9
quasar987 said:
In the book I took the formula from, they say it can be shows that if, at any time, the universe had a positive/negative/zero C, then it has always been so and will always be. In other words, the universe CANNOT change from open to flat to closed.

Another thing that's bugging me is, if the vacuum has density, then it should be subject to gravitationnal attraction, shouldn't it? I never heard anyone mention that though.

You have to look for the perfect solution for the vacuum(bubble nucleation/topology)? :smile:

Also you must understand why the universe is flat. Temperature is very important attribute that helps you consider?
 
  • #10
WMAP data indicates it is as flat as a pancake.
 
  • #11
Why does everyone try to make a simple problem so difficult?

>WMAP data indicates it is as flat as a pancake.<

The background radiation observation only tells you that, the universe if uniform to a high degree except for clumping. You will see the same result if the universe has a flat or curved geometry.

Everyone is always trying to make the universe fit his or her theory. It must in the end be the other way around

You must first decide if you accept the idea of the Big Bang.

If you don’t then you have the problem of explaining all the observations that support the Big Bang theory. Up to this point I have seen no other theory that works.

If you accept the Big Bang theory then you accept the concept of expansion outward from the Big Bang. With out going into detail about the early universe and the resulting mass.

You must then accept that the mass that is the result of the Big Bang moved outward from the center in all directions. This resulted in a three dimensional spatial sphere. If you problem is not being able to visualize a three dimensional sphere you are not alone. The lack of visualization does not change the way the universe is.

If you think the universe is geometrically flat then you must explain how the edges where able to move faster from the center of the BB to form a flat surface. That same surface must also be a three dimensional surface. You have not eliminated the three dimensional surface.

There is no problem with mass affecting the shape of the universe. All the mass of the universe moved out uniformly in all directions and only affected mass space in local areas. This is observed by the uniform distribution, over a large area, of objects in the sky. You note that I use the term mass space. Mass only affects the force of mass, gravity. Mass does not affect the electric force and the electric force does not affect mass. Therefore mass does not curve space it only curves space that affects mass.

>Another thing that's bugging me is, if the vacuum has density, then it should be subject to gravitational attraction, shouldn't it? I never heard anyone mention that though.<

The vacuum density, aether, or all prevailing medium APM. Or what ever you want to call it is not a mass construct. Just as the electric charge has a different force than mass. The APM is not required to have any force at all.

There is nothing wrong with an open universe. The universe will just fade away until all energy differentials are below the Planck level.

There is more problem with a closed universe. What happen to the idea of escape velocity? The force of gravity decreases a square, as the increase of expansion is linear.
 
  • #12
quasar987 said:
What is actually commonly accepted in the cosmologist society regarding the model of the universe? Do they think C=0 or > 0 or < 0 ? And what makes them think that?


Also, how do one get the shapes related to each posibility for C from the equations of GR?

the run of mill working cosmologists think it is absolutely flat or just slightly positive curvature

with your equations you are basically saying
Is the actual density (including cosm. const Lambda) bigger than or equal to or less than the critical density?

the customary thing for cosmologists is not to take the difference in the densities and say is it positive zero or negative but to take the ratio
of
real-rho divided by critical-rho
and call that ratio Omega
and then ask is Omega bigger than 1 or just exactly equal 1 or less.

(you can see it is different way of saying same thing)

and then the WMAP data is saying so far that
Omega = 1.02 +/- 0.02

do you want a link to the WMAP report?

so you can see it is not conclusive. Omega could be exactly 1, or it might be slightly bigger. (spatial flatness or slight positive curvature)
 
  • #13
What were the chances of that happening ( 1.02 +- 0.02) ?
Unlucky if you like a clear outcome.
 
  • #14
marcus said:
the customary thing for cosmologists is not to take the difference in the densities and say is it positive zero or negative but to take the ratio
of
real-rho divided by critical-rho
and call that ratio Omega
and then ask is Omega bigger than 1 or just exactly equal 1 or less.

(you can see it is different way of saying same thing)

and then the WMAP data is saying so far that
Omega = 1.02 +/- 0.02

do you want a link to the WMAP report?

so you can see it is not conclusive. Omega could be exactly 1, or it might be slightly bigger. (spatial flatness or slight positive curvature)


The 3D Universe


Open ([tex]\omega[/tex]<1) Hyperbolic geometry

Flat (([tex]\omega[/tex]=1) Euclidean geometry

Closed ([tex]\omega[/tex]>1) Spherical geometry
 
Last edited:
  • #15
I think omega is exactly 1. Observational evidence leans toward a slightly larger value [e.g., an open universe], but, if you apply thermodynamic laws to the universe as a whole [blackbody], 1 is the only result that is consistent with both thermodynamics and relativity, as far as I can see.
 
  • #16
If one wants to understand what has happened in the early universe, and the dynamical changes that this universe has gone through, what would have been appropriately considered as I said in the temperatures values?

What and how can we geometrically realize the process unfolding, is given by example currently in how we percieve the information in Gamma ray detection of these bursts?

Question then would be raised as to what shape the universe was in the begining, and what have we realized today? This transformative change is very simplistic in its consideration. :smile:
 

1. What is the general curvature of space?

The general curvature of space is a concept in the field of theoretical physics that describes the shape of the universe. It is a measure of how space is curved or bent due to the presence of matter and energy.

2. How is the general curvature of space measured?

The general curvature of space is measured using mathematical models, such as the Einstein field equations, which describe the relationship between the distribution of matter and energy and the curvature of space.

3. What does the general curvature of space tell us about the universe?

The general curvature of space can tell us about the overall geometry and structure of the universe. It can also provide insights into the expansion of the universe and the formation of large-scale structures such as galaxies and galaxy clusters.

4. How does the general curvature of space relate to Einstein's theory of general relativity?

Einstein's theory of general relativity is the foundation for understanding the general curvature of space. It describes how matter and energy affect the curvature of space and how this curvature in turn affects the motion of matter and energy.

5. Can the general curvature of space change?

According to current theories, the general curvature of space is not a fixed value and can change over time. It is influenced by the distribution of matter and energy in the universe, which can change due to various factors such as the expansion of the universe and the formation of new structures.

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