Ranku
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Is the curvature index κ necessarily zero in a flat universe with cosmological constant?
The curvature index κ in a flat universe with a cosmological constant is definitively zero. In a Friedmann-Robertson-Walker-Lemaitre universe, if the density relative to critical density satisfies the equation 1 = Ω = Ω_r + Ω_m + Ω_Λ, then κ equals zero, indicating flat spatial curvature. The total mass/energy density of the universe is expressed as ρ_total = ρ_m + ρ_r + ρ_Λ, with critical density defined as ρ_crit = 3H²/(8πG). If ρ_total equals ρ_crit, the universe is flat.
PREREQUISITESAstronomers, cosmologists, and physics students interested in the dynamics of the universe and the implications of curvature and energy density in cosmological models.
Yes. If a Friedmann-Robertson-Walker-Lemaitre universes has density (relative to critical density) ##1 = \Omega = \Omega_r + \Omega_r +\Omega_\Lambda##, then it is flat and ##\kappa = 0##. ("Flat" refers to spatial curvature (of 3-dimensional hypersurfaces), not to spacetime curvature.)Ranku said:Is the curvature index κ necessarily zero in a flat universe with cosmological constant?
To extend the discussion, the curvature index ##\kappa## can also cast in terms of its energy densityGeorge Jones said:Yes. If a Friedmann-Robertson-Walker-Lemaitre universes has density (relative to critical density) ##1 = \Omega = \Omega_r + \Omega_r +\Omega_\Lambda##, then it is flat and ##\kappa = 0##. ("Flat" refers to spatial curvature (of 3-dimensional hypersurfaces), not to spacetime curvature.)
No.Ranku said:To extend the discussion, the curvature index ##\kappa## can also cast in terms of its energy density
##\rho####\kappa#### =- \frac{3k}{8πGa^2}##. Can we identify the 'source' of ##\rho####\kappa##? Is it the matter density in the universe?