Taking the divergence of the linear Euler equation and defining the peculiar-velocity divergence gives
The assumption of negligible vorticity ensures that this longitudinal variable captures the velocity perturbation relevant to scalar density growth.
Solved by gpt-5.6-sol high.
Differentiate the linearized cosmological continuity equation, , and use :
Substitution of part (a), followed by the Poisson equation , yields
Solved by gpt-5.6-sol high.
For a barotropic equation of state, . A spatial Fourier mode of comoving wavenumber therefore satisfies
The Jeans wavenumber is defined by equality of the pressure and self-gravity terms:
For , pressure dominates and produces acoustic oscillations whose amplitude is affected by Hubble friction. For , self-gravity dominates and a growing mode develops: this is Jeans instability.
Solved by gpt-5.6-sol high.
Cold dark matter has . During matter domination,
The density equation becomes
Trying the power law gives
whose roots are and . Thus the cosmic-time matter density modes are
and the leading growing mode is .
Solved by gpt-5.6-sol high.
The constant-equation-of-state density scaling gives
For a spatially flat universe dominated by this component, the Friedmann equation gives . Integrating yields
This is accelerated expansion because .
Solved by gpt-5.6-sol high.
The dominant component is smooth, so only the subdominant matter density clusters. The cold-matter perturbation equation is therefore
At late times, , the source term is negligible compared with the expansion terms. Setting and using gives
It integrates to
The constant mode shows the suppression of matter growth by smooth accelerated expansion; the second mode decays.
Solved by gpt-5.6-sol high.

Articles by others on the same topic (0)

There are currently no matching articles.