Equations · equation

Cosmological Fluid Equation

Cosmology · 1927

Equation
ρ̇ + 3H(ρ + p/c²) = 0
Field
Cosmology
Named After
Georges Lemaître
Symbols
ρ energy density of a component · ρ̇ its rate of change with cosmic time · H = ȧ/a the Hubble parameter · p pressure · c speed of light
Year
1927

Significance

The third member of the Friedmann trio, and the one most often left out: energy conservation for an expanding universe. It is nothing more exotic than the first law of thermodynamics — dU = −p dV — applied to a comoving volume that is growing, which is why the pressure term appears alongside the density. Any two of the three cosmological equations imply the third, so this is the closure that makes the system solvable; without it the Friedmann equations have more unknowns than constraints.

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From the Equations database in Notion, last edited 2026-08-26. This page is the row, rendered by the build; nothing on it is written by hand.