Hubble's law

Hubble's law, also called the Hubble–Lemaître law, tells us that galaxies are moving away from Earth. The farther a galaxy is, the faster it moves away. We can learn how fast a galaxy is moving by looking at a change in the color of its light, called redshift.

An analogy for explaining Hubble's law, using raisins in a rising loaf of bread in place of galaxies. If a raisin is twice as far away from a place as another raisin, then the farther raisin would move away from that place twice as quickly.

This idea was first shared by Edwin Hubble in 1929, but others had noticed similar patterns before him. Georges Lemaître studied this in 1927 and estimated how fast the universe might be expanding. Hubble used measurements of how bright galaxies looked and their redshifts to find a better value for this speed.

Hubble's law is important because it was the first proof that the universe is expanding. This idea helps us understand the Big Bang, the event that started the universe. The law is shown by a simple equation that connects how far a galaxy is from us to how fast it is moving away. By studying this law, scientists have learned more about the age and size of our universe.

Discovery

Main article: Friedmann–Lemaître–Robertson–Walker metric

Three steps to the Hubble constant

Main article: Cosmological constant

Long before Edwin Hubble made his discoveries, scientists thought about whether the universe was growing or staying the same size. Some used special math created by Albert Einstein to show the universe might be changing size over time.

In 1912, an astronomer named Vesto Slipher saw that most distant objects called "spiral nebulae" (now called galaxies) were moving away from Earth. Ten years later, a scientist named Georges Lemaître used math to show how fast these galaxies might be moving apart. In the 1920s, Edwin Hubble used powerful telescopes to measure how far away these galaxies were. He found that the farther they were, the faster they seemed to move away — a discovery that changed how we understand the universe.

Interpretation

Hubble's law tells us that galaxies are moving away from Earth. The farther a galaxy is, the faster it moves away. We learn how fast a galaxy is moving by looking at how its light changes color, called redshift.

A variety of possible recessional velocity vs. redshift functions including the simple linear relation v = cz; a variety of possible shapes from theories related to general relativity; and a curve that does not permit speeds faster than light in accordance with special relativity. All curves are linear at low redshifts.

Scientists use a simple formula for this. The speed at which a galaxy moves away (called its recessional velocity) depends on a number (called Hubble's constant) and the distance to the galaxy. This helps us understand how the universe is expanding. Even galaxies very far away can move away from us faster than the speed of light because space itself is stretching.

The universe is expanding faster over time. This means galaxies will keep moving farther away from each other.

Derivation of the Hubble parameter

Start with the Friedmann equation:

H² ≡ ( ȧ⁄a )² = 8πG⁄3 ρ − kc²⁄a² + Λc²⁄3,

where H is the Hubble parameter, a is the scale factor, G is the gravitational constant, k is the shape of the universe and equal to −1, 0, or 1, and Λ is the cosmological constant.

If the universe is matter-dominated, then the amount of matter ρ should be taken to include just matter so

ρ = ρ_m0⁄a³,

where ρ_m0 is the amount of matter today. From the Friedmann equation we know that for matter, its amount decreases as the universe grows, so the equation above must be true. We can also define (see density parameter for Ω_m)

ρ_c = 3H₀²⁄8πG; Ω_m ≡ ρ_m0⁄ρ_c = 8πG⁄3H₀² ρ_m0;

therefore:

ρ = ρ_c Ω_m⁄a³.

Also, by definition, Ω_k ≡ −kc²⁄(a₀H₀)² Ω_Λ ≡ Λc²⁄3H₀²,

where the subscript 0 refers to the values today, and a₀ = 1. Substituting all of this into the Friedmann equation at the start of this section and replacing a with a = 1⁄(1+z) gives

H²(z) = H₀² ( Ω_m(1+z)³ + Ω_k(1+z)² + Ω_Λ ) .

If the universe is both matter-dominated and dark energy-dominated, then the above equation for the Hubble parameter will also be a function of the equation of state of dark energy. So now:

ρ = ρ_m(a) + ρ_de(a),

where ρ_de is the amount of the dark energy. If dark energy derives from a cosmological constant such as that introduced by Einstein, it can be shown that w = −1. The equation then reduces to the last equation in the matter-dominated universe section, with Ω_k set to zero. In that case the initial dark energy amount ρ_de0 is given by

ρ_de0 = Λc²⁄8πG, Ω_de = Ω_Λ.

Units derived from the Hubble constant

The Hubble constant has units that help us understand time in the universe. The Hubble time is the opposite of the Hubble constant. It gives an idea of how old the universe might be if its expansion had stayed the same. It is about 14.4 billion years, a little more than the actual age of the universe, which is around 13.8 billion years.

Another important unit is the Hubble length. This is the distance light can travel during the Hubble time. This distance is about 14.4 billion light years. It tells us how far away galaxies are that are moving away from us at the speed of light. The Hubble volume refers to a part of the universe that has this size, though its exact meaning can vary among scientists.

Determining the Hubble constant

The Hubble constant, shown as H₀, is a key number that helps us understand how fast the universe is expanding. We can't measure it directly, but scientists use observations of stars and other objects in space to estimate its value.

In the past, scientists used bright stars called Cepheid variable stars to measure distances in space. One famous astronomer, Walter Baade, discovered that there were two types of these stars, which helped change our understanding of the size of the universe. Today, there is still some difference between measurements made using different techniques. Scientists are working to understand why these differences exist and what they might tell us about the universe.

Measurements of the Hubble constant

The Hubble–Lemaître law tells us that galaxies move away from us. The farther they are, the faster they move. Scientists measure how fast these galaxies are moving by looking at the light they give off. This light changes color in a way that shows their speed.

Many careful measurements have been made to find the exact number, called the Hubble constant. This number helps us understand how quickly the universe is growing. It is important for learning about the age and size of our universe.

Main article: Hubble's law

Date published	Hubble constant (km/s)/Mpc	Observer	Remarks / methodology
2026-04-01	73.50±0.81	H0DN Collaboration	The Local Distance Network: A community consensus report
2025-05-27	70.39±1.94	W. Freedman et al	Tip of the Red Giant Branch (TRGB) method (values from J-Region Asymptotic Giant Branch (JAGB) and Cepheids also reported)(JWST and HST data)
2025-01-14	75.7+8.1 −5.5	Pascale et al.	Timing delay of gravitationally lensed images of Supernova H0pe. Independent of cosmic distance ladder or the CMB. JWST data. (2023-05-11 cell and this one are the only 2 values with this method so far)
2024-12-01	72.6±2.0	SH0ES+CCHP JWST	JWST, 3 methods, Cepheids, TRGB, JAGB, 2 groups data
2023-07-19	67.0±3.6	Sneppen et al.	Due to the blackbody spectra of the optical counterpart of neutron-star mergers, these systems provide strongly constraining estimators of cosmic distance.
2023-07-13	68.3±1.5	SPT-3G	CMB TT/TE/EE power spectrum. Less than 1σ discrepancy with Planck.
2023-05-11	66.6+4.1 −3.3	P. L. Kelly et al.	Timing delay of gravitationally lensed images of Supernova Refsdal. Independent of cosmic distance ladder or the CMB.
2022-12-14	67.3+10.0 −9.1	S. Contarini et al.	Statistics of cosmic voids using BOSS DR12 data set.
2022-02-08	73.4+0.99 −1.22	Pantheon+	SN Ia distance ladder (+SH0ES)
2022-06-17	75.4+3.8 −3.7	T. de Jaeger et al.	Use Type II supernovae as standardisable candles to obtain an independent measurement of the Hubble constant—13 SNe II with host-galaxy distances measured from Cepheid variables, the tip of the red giant branch, and geometric distance (NGC 4258).
2021-12-08	73.04±1.04	SH0ES	Cepheids-SN Ia distance ladder (HST+Gaia EDR3+"Pantheon+"). 5σ discrepancy with planck.
2021-09-17	69.8±1.7	W. Freedman	Tip of the red-giant branch (TRGB) distance indicator (HST+Gaia EDR3)
2020-12-16	72.1±2.0	Hubble Space Telescope and Gaia EDR3	Combining earlier work on red giant stars, using the tip of the red-giant branch (TRGB) distance indicator, with parallax measurements of Omega Centauri from Gaia EDR3.
2020-12-15	73.2±1.3	Hubble Space Telescope and Gaia EDR3	Combination of HST photometry and Gaia EDR3 parallaxes for Milky Way Cepheids, reducing the uncertainty in calibration of Cepheid luminosities to 1.0%. Overall uncertainty in the value for H₀ is 1.8%, which is expected to be reduced to 1.3% with a larger sample of type Ia supernovae in galaxies that are known Cepheid hosts. Continuation of a collaboration known as Supernovae, H₀, for the Equation of State of Dark Energy (SHoES).
2020-12-04	73.5±5.3	E. J. Baxter, B. D. Sherwin	Gravitational lensing in the CMB is used to estimate H₀ without referring to the sound horizon scale, providing an alternative method to analyze the Planck data.
2020-11-25	71.8+3.9 −3.3	P. Denzel et al.	Eight quadruply lensed galaxy systems are used to determine H₀ to a precision of 5%, in agreement with both "early" and "late" universe estimates. Independent of distance ladders and the cosmic microwave background.
2020-11-07	67.4±1.0	T. Sedgwick et al.	Derived from 88 0.02 H₀ estimate is corrected for the effects of peculiar velocities in the supernova environments, as estimated from the galaxy density field. The result assumes Ω_m = 0.3, Ω_Λ = 0.7 and a sound horizon of 149.3 Mpc, a value taken from Anderson et al. (2014).
2020-09-29	67.6+4.3 −4.2	S. Mukherjee et al.	Gravitational waves, assuming that the transient ZTF19abanrh found by the Zwicky Transient Facility is the optical counterpart to GW190521. Independent of distance ladders and the cosmic microwave background.
2020-06-18	75.8+5.2 −4.9	T. de Jaeger et al.	Use Type II supernovae as standardisable candles to obtain an independent measurement of the Hubble constant—7 SNe II with host-galaxy distances measured from Cepheid variables or the tip of the red giant branch.
2020-02-26	73.9±3.0	Megamaser Cosmology Project	Geometric distance measurements to megamaser-hosting galaxies. Independent of distance ladders and the cosmic microwave background.
2019-10-14	74.2+2.7 −3.0	STRIDES	Modelling the mass distribution & time delay of the lensed quasar DES J0408-5354.
2019-09-12	76.8±2.6	SHARP/H0LiCOW	Modelling three galactically lensed objects and their lenses using ground-based adaptive optics and the Hubble Space Telescope.
2019-08-20	73.3+1.36 −1.35	K. Dutta et al.	This H 0 {\displaystyle H_{0}} is obtained analysing low-redshift cosmological data within ΛCDM model. The datasets used are type-Ia supernovae, baryon acoustic oscillations, time-delay measurements using strong-lensing, H(z) measurements using cosmic chronometers and growth measurements from large scale structure observations.
2019-08-15	73.5±1.4	M. J. Reid, D. W. Pesce, A. G. Riess	Measuring the distance to Messier 106 using its supermassive black hole, combined with measurements of eclipsing binaries in the Large Magellanic Cloud.
2019-07-16	69.8±1.9	Hubble Space Telescope	Distances to red giant stars are calculated using the tip of the red-giant branch (TRGB) distance indicator.
2019-07-10	73.3+1.7 −1.8	H0LiCOW collaboration	Updated observations of multiply imaged quasars, now using six quasars, independent of the cosmic distance ladder and independent of the cosmic microwave background measurements.
2019-07-08	70.3+5.3 −5.0	The LIGO Scientific Collaboration and The Virgo Collaboration	Uses radio counterpart of GW170817, combined with earlier gravitational wave (GW) and electromagnetic (EM) data.
2019-03-28	68.0+4.2 −4.1	Fermi-LAT	Gamma ray attenuation due to extragalactic light. Independent of the cosmic distance ladder and the cosmic microwave background.
2019-03-18	74.03±1.42	Hubble Space Telescope	Precision HST photometry of Cepheids in the Large Magellanic Cloud (LMC) reduce the uncertainty in the distance to the LMC from 2.5% to 1.3%. The revision increases the tension with CMB measurements to the 4.4σ level (P=99.999% for Gaussian errors), raising the discrepancy beyond a plausible level of chance. Continuation of a collaboration known as Supernovae, H₀, for the Equation of State of Dark Energy (SHoES).
2019-02-08	67.78+0.91 −0.87	Joseph Ryan et al.	Quasar angular size and baryon acoustic oscillations, assuming a flat ΛCDM model. Alternative models result in different (generally lower) values for the Hubble constant.
2018-11-06	67.77±1.30	Dark Energy Survey	Supernova measurements using the inverse distance ladder method based on baryon acoustic oscillations.
2018-09-05	72.5+2.1 −2.3	H0LiCOW collaboration	Observations of multiply imaged quasars, independent of the cosmic distance ladder and independent of the cosmic microwave background measurements.
2018-07-18	67.66±0.42	Planck Mission	Final Planck 2018 results.
2018-04-27	73.52±1.62	Hubble Space Telescope and Gaia	Additional HST photometry of galactic Cepheids with early Gaia parallax measurements. The revised value increases tension with CMB measurements at the 3.8σ level. Continuation of the SHoES collaboration.
2018-02-22	73.45±1.66	Hubble Space Telescope	Parallax measurements of galactic Cepheids for enhanced calibration of the distance ladder; the value suggests a discrepancy with CMB measurements at the 3.7σ level. The uncertainty is expected to be reduced to below 1% with the final release of the Gaia catalog. SHoES collaboration.
2017-10-16	70.0+12.0 −8.0	The LIGO Scientific Collaboration and The Virgo Collaboration	Standard siren measurement independent of normal "standard candle" techniques; the gravitational wave analysis of a binary neutron star (BNS) merger GW170817 directly estimated the luminosity distance out to cosmological scales. An estimate of fifty similar detections in the next decade may arbitrate tension of other methodologies. Detection and analysis of a neutron star-black hole merger (NSBH) may provide greater precision than BNS could allow.
2016-11-22	71.9+2.4 −3.0	Hubble Space Telescope	Uses time delays between multiple images of distant variable sources produced by strong gravitational lensing. Collaboration known as H₀ Lenses in COSMOGRAIL's Wellspring (H0LiCOW).
2016-08-04	76.2+3.4 −2.7	Cosmicflows-3	Comparing redshift to other distance methods, including Tully–Fisher, Cepheid variable, and Type Ia supernovae. A restrictive estimate from the data implies a more precise value of 75±2.
2016-07-13	67.6+0.7 −0.6	SDSS-III Baryon Oscillation Spectroscopic Survey (BOSS)	Baryon acoustic oscillations. An extended survey (eBOSS) began in 2014 and is expected to run through 2020. The extended survey is designed to explore the time when the universe was transitioning away from the deceleration effects of gravity from 3 to 8 billion years after the Big Bang.
2016-05-17	73.24±1.74	Hubble Space Telescope	Type Ia supernova, the uncertainty is expected to go down by a factor of more than two with upcoming Gaia measurements and other improvements. SHoES collaboration.
2015-02	67.74±0.46	Planck Mission	Results from an analysis of Planck's full mission were made public on 1 December 2014 at a conference in Ferrara, Italy. A full set of papers detailing the mission results were released in February 2015.
2013-10-01	74.4±3.0	Cosmicflows-2	Comparing redshift to other distance methods, including Tully–Fisher, Cepheid variable, and Type Ia supernovae.
2013-03-21	67.80±0.77	Planck Mission	The ESA Planck Surveyor was launched in May 2009. Over a four-year period, it performed a significantly more detailed investigation of cosmic microwave radiation than earlier investigations using HEMT radiometers and bolometer technology to measure the CMB at a smaller scale than WMAP. On 21 March 2013, the European-led research team behind the Planck cosmology probe released the mission's data including a new CMB all-sky map and their determination of the Hubble constant.
2012-12-20	69.32±0.80	WMAP (9 years), combined with other measurements
2010	70.4+1.3 −1.4	WMAP (7 years), combined with other measurements	These values arise from fitting a combination of WMAP and other cosmological data to the simplest version of the ΛCDM model. If the data are fit with more general versions, H₀ tends to be smaller and more uncertain: typically around 67±4 (km/s)/Mpc although some models allow values near 63 (km/s)/Mpc.
2010	71.0±2.5	WMAP only (7 years).
2009-02	70.5±1.3	WMAP (5 years), combined with other measurements
2009-02	71.9+2.6 −2.7	WMAP only (5 years)
2007	70.4+1.5 −1.6	WMAP (3 years), combined with other measurements
2006-08	76.9+10.7 −8.7	Chandra X-ray Observatory	Combined Sunyaev–Zeldovich effect and Chandra X-ray observations of galaxy clusters. Adjusted uncertainty in table from Planck Collaboration 2013.
2003	72±5	WMAP (First year) only
2001-05	72±8	Hubble Space Telescope Key Project	This project established the most precise optical determination, consistent with a measurement of H₀ based upon Sunyaev–Zel'dovich effect observations of many galaxy clusters having a similar accuracy.
before 1996	50 — 90 (est.)
1994	67±7	Supernova 1a Light Curve Shapes	Determined relationship between luminosity of SN 1a's and their Light Curve Shapes. Riess et al. used this ratio of the light curve of SN 1972E and the Cepheid distance to NGC 5253 to determine the constant.
mid 1970's	100±10	Gérard de Vaucouleurs	De Vaucouleurs believed he had improved the accuracy of Hubble's constant from Sandage's because he used 5x more primary indicators, 10× more calibration methods, 2× more secondary indicators, and 3× as many galaxy data points to derive his 100±10.
early 1970s	55 (est.)	Allan Sandage and Gustav Tammann
1958	75 (est.)	Allan Sandage	This was the first good estimate of H₀, but it would be decades before a consensus was achieved.
1956	180	Humason, Mayall and Sandage
1929	500	Edwin Hubble, Hooker telescope
1927	625	Georges Lemaître	First measurement and interpretation as a sign of the expansion of the universe.