Why is the non-zero value of spatial curvature +/- 1?

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The discussion centers on the relationship between spatial curvature and the curvature parameter k in Friedmann's equations. It is noted that when space is flat, the radius of curvature is infinite, leading to a vanishing spatial curvature. The value of |k| being equal to 1 when space is not flat is explained as a convention where k represents a ratio related to the radius of curvature. The radius of curvature is influenced by the scale factor, which scales distances in the universe, and is also connected to the curvature constant Ω_k. Understanding these concepts is crucial for grasping the dynamics of the universe's geometry.
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Going from the Newtonian to relativistic version of Friedmann's equation we use the substitution
kc^{2} = -\frac{2U}{x^{2}}

The derivation considers the equation of motion of a particle with classic Newtonian dynamics. I can sought of see that if space is flat the radius of curvature will be infinite, so spatial curvature will vanish, but why exactly is |k| = 1 when space is not flat ?

Also I'm guessing that k is actually a ratio of something over that things absolute value, e.g.
k = \frac{thing}{\|thing\|}, because why else would it be +/- 1 or 0?
 
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sunrah said:
but why exactly is |k| = 1 when space is not flat ?
It's purely a convention. By this convention, when k = \pm 1, the scale factor is the radius of curvature.

An alternative convention is to set the scale factor equal to 1 today. With this convention, the curvature parameter can take on any value, and is proportional to the inverse of the radius of curvature squared.
 
Thanks, do you know where I can learn more about his? The introductory cosmology books just state this without justifying it and that bugs me.
 
So the radius of curvature is a function of the scale factor, but why? That's what I'd like to know. It isn't obvious to me. Thanks
 
sunrah said:
So the radius of curvature is a function of the scale factor, but why? That's what I'd like to know. It isn't obvious to me. Thanks
If the universe is described by a sphere, then the radius of curvature is the radius of the sphere. If you increase the distances between every two objects by a factor of two, you increase the radius of the sphere by a factor of two, and therefore increase the radius of curvature by a factor of two.
 
That only works for a finite universe. But, then again, Einstein strongly favored that option having realized his field equations are not well behaved in the presence of infinities.
 
sunrah said:
So the radius of curvature is a function of the scale factor, but why?
Actually, it is a function of the curvature constant \Omega_k= 1-\Omega_{total}. The scale factor is just what it says, something to scale the effect of all the Omegas to earlier times. For a small positive curvature (i.e. a small negative curvature constant, unfortunately, due to legacy) the radius of spatial curvature is R_k \approx R_{Hubble}/\sqrt{\Omega_{total} - 1}. For spatially flat it blows up to infinity and for a spatially open universe it comes out as an imaginary number.
 
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