Universe Expansion Calculator

Calculate the Hubble parameter, cosmological distances, and scale factor from redshift and flat-universe density parameters.

Calculate cosmic expansion
Enter redshift, Hubble constant, matter and dark-energy density, and a reference lookback time.

About universe expansion

Cosmic expansion describes the growth of distances between widely separated, gravitationally unbound regions of the universe. Redshift z records how much a photon's wavelength has stretched since emission, while the scale factor at emission is a = 1/(1 + z). The Hubble constant H₀ describes the present expansion rate in kilometres per second per megaparsec. It does not mean every object is flying through static space at a speed proportional to distance; in cosmology, the geometry of space evolves, and nearby bound systems do not participate in the expansion in the same way. This calculator uses a flat matter-plus-dark-energy model. At a selected redshift, the expansion rate is H(z) = H₀√[Ωm(1 + z)³ + ΩΛ]. Matter becomes dynamically more important toward the past because its density scales with the inverse cube of the scale factor, whereas a cosmological constant retains constant density. Typical present-day illustrative parameters are Ωm near 0.3 and ΩΛ near 0.7. Radiation and curvature are omitted, so the model is most useful at modest redshift and when the supplied density parameters represent an approximately flat universe. Distance in an expanding universe has several definitions. The line-of-sight comoving distance preserves present-day coordinate separation and is calculated from c/H₀ times the numerical integral of 1/E(z). This page evaluates that integral with Simpson's rule. Luminosity distance is (1 + z) times comoving distance and connects an object's intrinsic luminosity to its observed flux. Angular-diameter distance, which is not displayed here, would divide comoving distance by (1 + z). These distances agree closely only for nearby sources, so choosing the definition appropriate to an observation is essential. The lookback-time field is shown as a reference value because reproducing it independently requires another cosmological integral and assumptions about all energy components. It can be used to annotate an example or compare an externally obtained age estimate with the distance results. The output is educational rather than a precision cosmology pipeline. High-redshift work should include radiation, neutrinos, curvature where appropriate, parameter covariance, and rigorously controlled numerical methods. Published research also distinguishes proper, comoving, luminosity, and angular distances carefully. For observational analysis, use current survey parameters, established cosmology libraries, uncertainty propagation, and peer-reviewed methods rather than treating a single calculator result as a measurement.

Universe expansion examples

Representative redshifts illustrate how expansion rate and cosmological distance grow.

CosmologyRepresentative resultObject scale
z = 0.1, H₀ = 70, Ωm = 0.3, ΩΛ = 0.7H(z) ≈ 73.4 km/s/MpcNearby galaxy
z = 1, H₀ = 70, Ωm = 0.3, ΩΛ = 0.7H(z) ≈ 123.2 km/s/MpcIntermediate redshift
z = 3, H₀ = 70, Ωm = 0.3, ΩΛ = 0.7H(z) ≈ 312.3 km/s/MpcDistant quasar

How to calculate expansion metrics

  1. Enter the observed redshift as a nonnegative value.
  2. Enter a Hubble constant and compatible matter and dark-energy density parameters.
  3. Add a reference lookback time if one is available from your source.
  4. Select Calculate and compare H(z), comoving distance, luminosity distance, and scale factor.

Frequently asked questions

What does the Hubble constant measure?

It parameterizes the present relationship between cosmic distance and expansion recession rate. Its units are kilometres per second per megaparsec.

Does redshift equal velocity divided by light speed?

Only approximately at very small redshift. Cosmological and relativistic relationships become nonlinear as redshift grows.

Why are there different cosmological distances?

Expansion affects observations of angles, flux, and coordinate separation differently. Comoving and luminosity distances therefore serve different measurement purposes.

Should Ωm and ΩΛ add to one?

They add to one in the simplified flat model when other components are negligible. Radiation, curvature, and additional components require a broader equation.

Is the entered lookback time calculated here?

No. It is retained as a reference alongside the calculated expansion and distance outputs, avoiding an unsupported age claim from an incomplete model.