Calculate cosmological galaxy proper distances (\(d = v / H_0\)), recession velocities (\(v = H_0 \cdot d\)), spectroscopic redshifts (\(z\)), Hubble time (\(t_H = 1/H_0\)), and Hubble sphere horizons (\(R_H = c/H_0\)) with Planck 2018 vs. SH0ES Hubble tension modeling.
Select cosmological expansion model and input kinematic variables.
322.9 Million Light-Years • Lookback: 323 Myr
| 🌌 Proper Distance (\(d\)) | 99.00 Mpc |
| 🌟 Light-Years (\(\text{ly}\)) | 322.9 Mly |
| 🚀 Recession Velocity (\(v\)) | 6,930 km/s |
| ⚡ Velocity / Light Speed | 0.0231 c |
| 📐 Spectroscopic Redshift (\(z\)) | 0.0231 |
| ⏱️ Hubble Time (\(t_H\)) | 13.97 Gyr |
| 🌐 Hubble Horizon (\(R_H\)) | 4,283 Mpc |
| 🔭 Expansion Regime | Sub-luminal (\(v < c\)) |
First formulated observationally by Georges Lemaître (1927) and Edwin Hubble (1929), Hubble's Law describes the fundamental observational relationship of physical cosmology: distant galaxies recede from us at speeds directly proportional to their distance: $$v = H_0 \times d$$
Cosmological distances, recession speeds, and lookback times computed at \(H_0 = 70.0\,\text{km/s/Mpc}\).
| Cosmic Landmark | Distance (Mpc) | Distance (Mly) | Recession Speed (\(v\)) | Redshift (\(z\)) | Lookback Time |
|---|---|---|---|---|---|
| Virgo Cluster (M87) | \(16.5\,\text{Mpc}\) | \(53.8\,\text{Mly}\) | \(1,155\,\text{km/s}\) | \(0.00385\) | \(53.8\,\text{Million Years}\) |
| Fornax Cluster | \(19.0\,\text{Mpc}\) | \(62.0\,\text{Mly}\) | \(1,330\,\text{km/s}\) | \(0.00444\) | \(62.0\,\text{Million Years}\) |
| Centaurus Cluster | \(49.5\,\text{Mpc}\) | \(161.4\,\text{Mly}\) | \(3,465\,\text{km/s}\) | \(0.01156\) | \(161.4\,\text{Million Years}\) |
| Coma Cluster (Abell 1656) | \(99.0\,\text{Mpc}\) | \(322.9\,\text{Mly}\) | \(6,930\,\text{km/s}\) | \(0.02312\) | \(322.9\,\text{Million Years}\) |
| Hercules Supercluster | \(200.0\,\text{Mpc}\) | \(652.3\,\text{Mly}\) | \(14,000\,\text{km/s}\) | \(0.04670\) | \(652.3\,\text{Million Years}\) |
| Hubble Sphere Horizon | \(4,283\,\text{Mpc}\) | \(13.97\,\text{Gly}\) | \(299,792\,\text{km/s}\) (\(c\)) | \(1.41\) | \(9.1\,\text{Billion Years}\) |
The geometric baseline. Trigonometric parallax measured by the ESA Gaia space observatory provides direct distances up to \(\sim 10\,\text{kpc}\) across the Milky Way.
Standard candles. Henrietta Leavitt's Period-Luminosity law links pulsation periods to intrinsic brightness, anchoring distances to nearby spiral galaxies up to \(30\text{--}40\,\text{Mpc}\).
Thermonuclear standardizable candles ($M_B \approx -19.3$). Visible across billions of light-years, these enabled the 1998 discovery of Dark Energy and accelerating cosmic expansion.
Galaxies are not moving *through* static space; rather, the continuous creation of metric space expands the distance between gravitationally unbound objects. As photons travel through expanding space, their wavelengths are stretched cosmologically: \(1 + z = a_0 / a(t)\).
Every galaxy also possesses a local kinematic velocity (\(v_{\text{pec}} \sim 100\text{--}600\,\text{km/s}\)) driven by local gravitational tugs (e.g., the Great Attractor). Observed velocity is \(v_{\text{obs}} = H_0 d + v_{\text{pec}}\). For nearby galaxies (\(d < 15\,\text{Mpc}\)), peculiar velocity can obscure the pure Hubble flow.
Because both measurement methodologies possess rigorous systematic checks, this \(> 5\sigma\) divide indicates that standard flat \(\Lambda\text{CDM}\) cosmology may require exciting new physics—such as Early Dark Energy, decaying dark matter, or modified gravity theories.
Authoritative answers to common questions about Hubble's Law, galaxy recession speeds, the Hubble Constant, and the cosmological distance ladder.