Nearby galaxy: z = 0.1
Input: z = 0.1. Result: age ≈ 12.459 Gyr, lookback ≈ 1.345 Gyr, comoving distance ≈ 432.6 Mpc. The low-redshift velocity shortcut is only an approximation; the integral supplies the model distance.
Choose redshift for a direct calculation, or another quantity to solve numerically for z.
Range: 0 to 20,000. Redshift is dimensionless.
Presets assume ΛCDM and set ΩΛ for spatial flatness after radiation. The local-H₀ option is a sensitivity example, not a complete survey fit.
20–150 km/s/Mpc.
Matter density, 0–2.
Vacuum density, −1 to 2.
Radiation is calculated as ΩR = 4.165 × 10−5/h²; curvature is ΩK = 1 − ΩM − ΩΛ − ΩR.
Keyboard shortcut: Ctrl/Cmd + Enter.
Both axes use log(1 + value) scaling so early cosmic time and very large distances remain visible together. Times are in Gyr; distances are in Gpc. Use the checkboxes to hide series. Focus a highlighted point for its exact value.
These reproducible examples use this page’s default Planck 2018 approximation.
Input: z = 0.1. Result: age ≈ 12.459 Gyr, lookback ≈ 1.345 Gyr, comoving distance ≈ 432.6 Mpc. The low-redshift velocity shortcut is only an approximation; the integral supplies the model distance.
Input: z = 3. Result: age ≈ 2.148 Gyr, lookback ≈ 11.656 Gyr, comoving distance ≈ 6.513 Gpc. Its present-day comoving distance exceeds 11.656 billion light-years because space expanded while the light traveled.
Input: z = 1100. Result: age ≈ 0.367 Myr, lookback ≈ 13.804 Gyr, comoving distance ≈ 13.908 Gpc. This is a background-expansion estimate, not a recombination-physics simulation.
| Redshift | Universe age then | Lookback time | Comoving distance today |
|---|---|---|---|
| 0 | 13.804 Gyr | 0 | 0 |
| 0.1 | 12.459 Gyr | 1.345 Gyr | 0.433 Gpc |
| 1 | 5.863 Gyr | 7.941 Gyr | 3.398 Gpc |
| 3 | 2.148 Gyr | 11.656 Gyr | 6.513 Gpc |
| 6 | 0.931 Gyr | 12.873 Gyr | 8.438 Gpc |
| 1100 | 0.367 Myr | 13.804 Gyr | 13.908 Gpc |
The calculator assumes an FLRW universe with matter, a cosmological constant, radiation, and curvature. These are model-dependent numerical integrals—not distance divided by the speed of light.
E(z) = H(z)/H₀ = √[ΩR(1+z)⁴ + ΩM(1+z)³ + ΩK(1+z)² + ΩΛ]
Lookback time: tL = H₀−1 ∫0z dz′ / [(1+z′)E(z′)]
Age at redshift: t(z) = H₀−1 ∫z∞ dz′ / [(1+z′)E(z′)] = H₀−1 ∫0a da′ / [a′E(a′)]
Line-of-sight comoving distance: DC = (c/H₀) ∫0z dz′ / E(z′)
Curvature: DM = (c/H₀)/√|ΩK| × Sk(√|ΩK|DCH₀/c), where Sk is sinh for ΩK > 0, its argument for ΩK = 0, and sin for ΩK < 0.
Derived measures: DA = DM/(1+z); DL = (1+z)DM; a = 1/(1+z); μ = 5 log₁₀(DL/Mpc) + 25.
Symbols: H₀ is today’s Hubble constant; H(z) is the expansion rate at z; c is light speed; ΩR, ΩM, ΩK, and ΩΛ are present-day radiation, matter, curvature, and vacuum density parameters; a is scale factor; DC is radial comoving distance; DM is transverse comoving distance; DA is angular-diameter distance; DL is luminosity distance.
Conversions: 1 Mpc = 3.26156 million light-years; 1 Gpc = 1,000 Mpc; c × 1 Gyr = 1 billion light-years. The inverse angular scale follows from 1 radian = 206,264.806 arcseconds.
Integrals use adaptive Simpson quadrature with a relative target near 10−8 and guarded recursion, replacing the former fixed 1,000-step sum. Reverse modes use bracketed bisection. The supported range is 0 ≤ z ≤ 20,000. Values normally settle well beyond the displayed precision.
The model includes ΩR = 4.165 × 10−5/h² and curvature. It assumes w = −1 and does not separately evolve massive neutrinos, changing dark energy, inhomogeneity, peculiar velocity, recombination, or measurement uncertainty. The default closes ΩΛ after its massless-radiation term, whereas Astropy Planck18 includes a 0.06 eV neutrino; that physical-model difference is larger than the integration error.
Checked 18 July 2026 against Astropy Planck18 (H₀ = 67.66, ΩM = 0.30966) and the equations/implementation described by Wright. This tool’s age and comoving distance differ from Astropy by at most about 0.21% across these checks, chiefly because of neutrino and closure treatment.
| z | Age: this tool | Age: Astropy | DC: this tool | DC: Astropy |
|---|---|---|---|---|
| 0 | 13.804 Gyr | 13.787 Gyr | 0 Mpc | 0 Mpc |
| 0.1 | 12.459 Gyr | 12.442 Gyr | 432.6 Mpc | 432.6 Mpc |
| 1 | 5.863 Gyr | 5.851 Gyr | 3398.4 Mpc | 3395.6 Mpc |
| 3 | 2.148 Gyr | 2.144 Gyr | 6512.6 Mpc | 6504.0 Mpc |
| 6 | 0.931 Gyr | 0.929 Gyr | 8437.8 Mpc | 8425.1 Mpc |
| 1100 | 0.367 Myr | 0.367 Myr | 13908.1 Mpc | 13886.3 Mpc |
Lookback time is the elapsed time between the emission of the light we observe and today. Multiplying it by c gives the light-travel distance, not the object's present-day separation.
The universe expanded while the light traveled. Lookback time records the travel duration, while comoving distance describes the object's present-day separation in the expanding coordinate system, so it can be much larger.
Use luminosity distance for flux and intrinsic-luminosity calculations. Use angular-diameter distance, or the reported kpc per arcsecond scale, to convert apparent angular size to physical size at emission.
Not generally. At very small redshift, cz approximates recession velocity, but at cosmological redshift the wavelength stretch mainly traces expansion and must be interpreted with a cosmological model.
Results depend on H0, matter, dark energy, curvature, radiation, neutrino treatment, and numerical method. Check that calculators use the same parameters and physical assumptions before comparing them.
Lookback time and all source distances are zero, scale factor is 1, and age at emission equals the present age of the universe. Distance modulus and angular scale are undefined at zero distance.
Planck 2018 is the best general default for standard flat Lambda-CDM comparisons. Choose WMAP9 to reproduce older literature, the illustrative local-H0 option to explore sensitivity, or Custom when a source specifies parameters.
Adaptive integration is numerically stable through z = 20000, but the physical model is simplified. Radiation is included, while massive neutrinos, evolving dark energy, and early-universe perturbation physics are not; at high z, model choice dominates rounding error.
Author and internal scientific-method reviewer: Starlight Robotics, publisher and maintainer of browser-based scientific calculation tools. Reviewed and updated . Numerical integration and reference values were checked during this review; no external individual reviewer is claimed.
The FLRW distance implementation follows the equations presented by Hogg and Wright; the adaptive integration, reverse solver, interface, and reference tests were independently implemented for this page.
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