Relativistic Cosmology and the Friedmann Equations
Einstein Equations in Cosmology
From Stress-Energy to Expansion
Assuming the FLRW metric and a perfect fluid with energy density and pressure , Einstein's equations reduce to the Friedmann equations: and Together with the continuity equation these determine the background evolution once an equation of state is specified.
Common Cosmic Fluids
| Component | Equation of state | Scaling with |
|---|---|---|
| Radiation | ||
| Matter | ||
| Curvature | effective | |
| Vacuum energy |
Acceleration Condition
Cosmic acceleration occurs when , so a sufficiently negative pressure component can drive .
For pressureless matter, how does the density scale with the scale factor?
Matter dilutes with volume, so .
Correct answer:
Critical Density and Density Parameters
The critical density is . Dimensionless density parameters are defined by , with curvature encoded by . The Friedmann equation can then be written as at a given epoch.
What condition defines a spatially flat universe in the Friedmann equation?
Flatness means the spatial slices have zero constant curvature.
Correct answer: The curvature term vanishes, corresponding to or equivalently .
Interpreting the Equation of State
Dust-like matter
- Pressure is negligible compared with energy density.
- Dominates structure formation at late times.
- Gives decelerating expansion in standard GR.
Dark energy
- Has sufficiently negative pressure.
- Can cause accelerated expansion.
- May be a cosmological constant or dynamical field.
Which term in the Friedmann equation can mimic a negative curvature-like contribution but is not geometric curvature?
A vacuum-energy term changes expansion dynamics without being spatial curvature.
Correct answer:
Deriving the First Friedmann Equation
-
1
Start from the FLRW metric and compute the Einstein tensor.
-
2
Insert a perfect-fluid stress-energy tensor into Einstein's equations.
-
3
Use the -component to isolate the expansion rate.
-
4
Identify the curvature, matter, radiation, and vacuum-energy contributions.
Research-Level Caveat
The background equations are exact only for an idealized homogeneous and isotropic spacetime; real cosmology requires perturbations, backreaction considerations, and observational averaging.