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Einstein Field Equations

The Einstein field equations G_μν = 8πG/c⁴ T_μν equate the geometry of spacetime (through the Einstein tensor G_μν built from the Riemann curvature tensor) with the distribution of energy and momentum (through the stress-energy tensor T_μν).

Key Concepts

  • Riemann tensor: R^ρ_μσν encodes spacetime curvature
  • Ricci tensor: R_μν = R^ρ_μρν (trace of Riemann)
  • Ricci scalar: R = g^μν R_μν
  • Einstein tensor: G_μν = R_μν - ½g_μν R
  • Cosmological constant Λ: G_μν + Λg_μν = 8πG/c⁴ T_μν

Key Equations

Einstein field equations
Gμν=Rμν12gμνR=8πGc4TμνG_{\mu\nu} = R_{\mu\nu} - \frac{1}{2}g_{\mu\nu}R = \frac{8\pi G}{c^4}T_{\mu\nu}
Bianchi identity
μGμν=0\nabla_\mu G^{\mu\nu} = 0
Weak-field limit
2Φ=4πGρ\nabla^2\Phi = 4\pi G\rho
Trace of EFE
R=8πGc4TR = -\frac{8\pi G}{c^4}T
Worked Example

Example Problem

Problem

In the weak-field limit, the 00 component of the EFE gives the Poisson equation ∇²Φ = 4πGρ. For a uniform sphere of density ρ=10³ kg/m³ and radius R=100 m, find ∇²Φ inside.

Solution

∇²Φ = 4πGρ = 4π×6.674×10⁻¹¹×10³ = 8.39×10⁻⁷ s⁻².

Practice

Exercises

7 problems
1 of 7

The constant 8πG/c⁴ in SI units. Find it in units of s²/(kg·m).

s²/(kg·m)
2 of 7

For a perfect fluid with T^μν = diag(ρc²,P,P,P), find the trace T = g_μν T^μν for the Minkowski metric (signs: -ρc²+3P). What is T for pressureless dust (P=0, ρ=1 kg/m³) in J/m³?

J/m³
3 of 7

The Schwarzschild radius r_s = 2GM/c². For the Earth (M=5.97×10²⁴ kg), find r_s in mm.

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4 of 7

The Schwarzschild radius of the Sun (M=2×10³⁰ kg) in km.

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5 of 7

The cosmological constant Λ ≈ 1.1×10⁻⁵² m⁻². The vacuum energy density is ρ_Λ = Λc²/(8πG). Find ρ_Λ in J/m³.

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6 of 7

The number of independent components of a 4×4 symmetric tensor in 4D spacetime.

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7 of 7

The Bianchi identity ensures ∇_μ G^μν = 0, implying ∇_μ T^μν = 0 (energy-momentum conservation). For a fluid with T^μν constant, ∂_μ T^μν = 0. For T^00=ρc²=10⁶ J/m³ uniform in space, ∂_0 T^00 + ∂_i T^i0 = 0. If T^i0=0 (no momentum flux), find ∂_0 T^00 (J/(m³·s)).

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Key Takeaways

  • The Einstein tensor G_μν encodes spacetime curvature from the Riemann tensor
  • The EFE equates curvature to energy-momentum content
  • In the weak-field limit, GR reduces to Newtonian gravity
  • The Bianchi identity guarantees local energy-momentum conservation