How an Inhomogeneous Sphere Expands: One Formula Instead of Complex Calculations ✛ ✎

Original: "Near universality of nonlinear transverse and radial velocity responses in spherical collapse with arbitrary radial profiles"
· Valerio Marra
arXiv:2608.27376v1 · 2026-08-27 · arXiv non-exclusive · independent analysis · 1 min
The expansion rate of any spherical region can be computed with a single simple formula.

A drop of ink spreads in a glass of water: its edges move faster than its center. Similarly, a clump of dark matter collapsing under its own gravity expands unevenly, with different shells flying apart at different speeds. Previously, astrophysicists could accurately describe only the simplest case: a homogeneous sphere with a sharp boundary. But real clumps are smooth: density gradually falls from the center to the edge, and each shell feels its own gravitational pull.

It turns out that the velocity perpendicular to the radius depends only on the mean density inside that point, while the velocity along the radius also depends on how quickly the density changes.

For quick estimates, a simple formula has been proposed that errs by no more than 0.7%. This means that instead of lengthy computer calculations, you can instantly obtain velocities for a given density profile. Previously, for each new profile you had to solve the equations of motion anew; now you just plug numbers into a ready-made formula.

For a shell in a void wall, the local contrast can be positive while the internal contrast is negative: the shell is denser than average, but inside it there is still a mass deficit. This difference drives the expansion anisotropy.

\delta h_\perp = -\frac{f}{3} A(\Delta)
The relative deviation of the transverse expansion rate from the background is proportional to the function A of the internal contrast
\delta h_\parallel = -\frac{f}{3} A(\Delta) - f [\delta - \Delta] A'(\Delta)
The radial response includes an additional term with the difference between local and internal contrasts, multiplied by the derivative of A
\Gamma = \frac{f [\Delta - \delta] A'(\Delta)}{1 - \frac{f}{3} \{ A(\Delta) + [\delta - \Delta] A'(\Delta) \}}
Dimensionless measure of the difference between radial and transverse rates
Concepts
cosmological homogeneity spatial curvature cosmological parameters density contrast Hubble's law hubble tension hubble flow density profile