sunrah
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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?
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?