Calculate astronomical redshift (\(z\)) and blueshift across Cosmological Expansion (FLRW metric & scale factor \(a\)), Relativistic Doppler Velocity (\(v/c\)), Gravitational Redshift (General Relativity), and Wavelength/Frequency Spectral Line Shifts.
Select a physical redshift formulation or enter observed spectral wavelengths.
v = 44,050 km/s • Scale Factor a = 0.864
| 🌌 Astronomical Redshift (\(z\)) | z = +0.1580 |
| 📐 Cosmic Scale Factor (\(a\)) | 0.8636 (86.4%) |
| 🚀 Relativistic Velocity (\(v\)) | 44,050 km/s (0.147 c) |
| 🏃 Classical Velocity (\(v = c z\)) | 47,367 km/s (0.158 c) |
| ⏳ Cosmic Lookback Time | 2.00 Gyr |
| ⏳ Universe Age at Emission | 11.79 Gyr |
| 📏 Comoving Distance (\(D_C\)) | 2.14 Gly (656 Mpc) |
| 💡 Luminosity Distance (\(D_L\)) | 2.48 Gly (760 Mpc) |
In observational astrophysics, a redshift (\(z\)) is not a single phenomenon, but arises from three fundamentally distinct physical mechanisms:
Light waves are stretched by the expanding metric of spacetime: \(1 + z = a_0 / a(t_{\text{em}})\). Photons travel across cosmic time expanding alongside the universe.
Physical motion of an object through local space: \(1 + z = \sqrt{\frac{1+\beta}{1-\beta}}\). Governed by Special Relativity and relativistic time dilation.
Photons lose kinetic energy escaping a dense gravitational well: \(1 + z = 1 / \sqrt{1 - \frac{2GM}{c^2 r}}\). Predicted by Einstein's General Relativity.
Laboratory rest-frame emission wavelengths and landmark cosmic shifts.
| Spectral Line | Rest \(\lambda_{\text{emit}}\) | Astronomical Landmark | Observed Redshift | Relativistic Velocity | Observed \(\lambda_{\text{obs}}\) |
|---|---|---|---|---|---|
| Hydrogen-Alpha (Hα) | \(656.28\,\text{nm}\) | Quasar 3C 273 | \(z = +0.158\) | \(44,050\,\text{km/s}\) | \(760.0\,\text{nm}\) (Near-IR) |
| Hydrogen-Beta (Hβ) | \(486.13\,\text{nm}\) | Andromeda Galaxy (M31) | \(z = -0.001001\) | \(-300\,\text{km/s}\) (Blueshift) | \(485.6\,\text{nm}\) (Blue) |
| Lyman-Alpha (Lyα) | \(121.57\,\text{nm}\) | Cosmic Noon Galaxy | \(z = +2.000\) | \(240,000\,\text{km/s}\) | \(364.7\,\text{nm}\) (Near-UV) |
| Lyman-Alpha (Lyα) | \(121.57\,\text{nm}\) | JWST JADES-GS-z14-0 | \(z = +14.32\) | \(0.991\,c\) | \(1,862.4\,\text{nm}\) (Infrared) |
| Hydrogen-Alpha (Hα) | \(656.28\,\text{nm}\) | Sirius B (White Dwarf) | \(z = +0.000297\) | \(+89\,\text{km/s}\) (Grav Shift) | \(656.47\,\text{nm}\) |
| Thermal Blackbody | \(966\,\text{nm}\) | CMB Recombination | \(z = +1089.9\) | Spacetime Expansion | \(1.053\,\text{mm}\) (Microwaves) |
Measured by dispersing light into a high-resolution spectrum to identify discrete atomic emission and absorption lines (such as \(\text{H}\alpha\), \(\text{H}\beta\), \(\text{Ly}\alpha\), \(\text{[O III]}\)). Yields extremely high precision (\(\Delta z / (1+z) \sim 10^{-4}\)), providing exact radial velocities and 3D cosmic mapping (e.g., SDSS, DESI).
Estimated from broad-band imaging filters (\(u, g, r, i, z, J, H, K\)) by matching Spectral Energy Distributions (SEDs) to known galactic templates. Detects prominent spectral breaks (the \(91.2\,\text{nm}\) Lyman break and the \(4000\,\text{\AA}\) Balmer break). Allows efficient survey measurements of hundreds of millions of galaxies simultaneously (e.g., Euclid, Vera C. Rubin LSST).
In Newtonian mechanics, the Doppler shift is approximated as \(z \approx v/c\). This linear approximation works well for slow-moving objects in our local galaxy (\(v < 0.1\,c\)). However, at higher redshifts (such as \(z = 2.0\)), the classical formula unphysically yields \(v = 2.0\,c\) (twice the speed of light)!
Special Relativity accounts for relativistic time dilation: $$v = c \cdot \frac{(1+z)^2 - 1}{(1+z)^2 + 1}$$ For \(z = 2.0\), the true relativistic Doppler velocity is \(v = 0.80\,c\) (\(240,000\,\text{km/s}\)), asymptotically approaching \(c\) as \(z \to \infty\) without ever violating the cosmic speed limit.
Authoritative answers to common questions about cosmological redshift, Doppler velocities, spectral line shifts, and gravitational time dilation.