# Gravity

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Attraction of masses and energy

For other uses, see [Gravity (disambiguation)](/source/Gravity_(disambiguation)).

"Gravitation" and "Law of Gravity" redirect here. For other uses, see [Gravitation (disambiguation)](/source/Gravitation_(disambiguation)) and [Law of Gravity (disambiguation)](/source/Law_of_Gravity_(disambiguation)).

The shapes of two massive [galaxies](/source/Galaxies) in this image evolved under the effects of gravity.

Part of a series on Classical mechanics F = d p d t {\displaystyle {\textbf {F}}={\frac {d\mathbf {p} }{dt}}} Second law of motion History Timeline Textbooks Branches Applied Celestial Continuum Dynamics Field theory Kinematics Kinetics Statics Statistical mechanics Fundamentals Acceleration Angular momentum Couple D'Alembert's principle Energy kinetic potential Force Frame of reference Inertial frame of reference Impulse Inertia / Moment of inertia Mass Mechanical power Mechanical work Moment Momentum Space Speed Time Torque Velocity Virtual work Formulations Newton's laws of motion Analytical mechanics Lagrangian mechanics Hamiltonian mechanics Routhian mechanics Hamilton–Jacobi equation Appell's equation of motion Koopman–von Neumann mechanics Core topics Damping Displacement Equations of motion Euler's laws of motion Fictitious force Friction Harmonic oscillator Inertial / Non-inertial reference frame Motion (linear) Newton's law of universal gravitation Newton's laws of motion Relative velocity Rigid body dynamics Euler's equations Simple harmonic motion Vibration Rotation Circular motion Rotating reference frame Centripetal force Centrifugal force reactive Coriolis force Pendulum Tangential speed Rotational frequency Angular acceleration / displacement / frequency / velocity Scientists Kepler Galileo Huygens Newton Horrocks Halley Maupertuis Daniel Bernoulli Johann Bernoulli Euler d'Alembert Clairaut Lagrange Laplace Poisson Hamilton Jacobi Cauchy Routh Liouville Appell Gibbs Koopman von Neumann Physics portal Category v t e

In physics, **gravity** (from [Latin](/source/Latin_language) *gravitas* 'weight'[1]), also known as **gravitation** or a **gravitational interaction**,[2] is a [fundamental interaction](/source/Fundamental_interaction), which may be described as the [force](/source/Force) that draws [material objects](/source/Physical_object) towards each other.

The gravitational attraction between clouds of primordial [hydrogen](/source/Hydrogen) and clumps of [dark matter](/source/Dark_matter) in the early [universe](/source/Universe) caused the hydrogen gas to [coalesce](/source/Coalescence_(physics)), eventually condensing and fusing to [form stars](/source/Star_formation). At larger scales this resulted in galaxies and clusters, so gravity is a primary driver for the large-scale structures in the universe. Gravity has an infinite range, although its effects become weaker as objects get farther away.

Gravity is described by the [general theory of relativity](/source/General_relativity), proposed by [Albert Einstein](/source/Albert_Einstein) in 1915, which describes gravity in terms of the [curvature](/source/Curvature) of [spacetime](/source/Spacetime), caused by the uneven distribution of mass. The most extreme example of this curvature of spacetime is a [black hole](/source/Black_hole), from which nothing—not even light—can escape once past the black hole's [event horizon](/source/Event_horizon).[3] However, for most applications, gravity is sufficiently well approximated by [Newton's law of universal gravitation](/source/Newton's_law_of_universal_gravitation), which describes gravity as an attractive force between any two bodies that is [proportional](/source/Proportionality_(mathematics)) to the product of their masses and [inversely proportional](/source/Inversely_proportional) to the [square](/source/Square_(algebra)) of the [distance](/source/Distance) between them.

Scientists are looking for a theory that describes gravity in the framework of [quantum mechanics](/source/Quantum_mechanics) ([quantum gravity](/source/Quantum_gravity)),[4] which would unify gravity and the other known fundamental interactions of physics in a single mathematical framework (a [theory of everything](/source/Theory_of_everything)).[5]

On the surface of a planetary body such as [on Earth](/source/Gravity_of_Earth), the force of gravity operates towards the center of the body and is modified by the centrifugal effects arising from the rotation of the body.[6] In this context, gravity gives [weight](/source/Weight) to physical objects and is essential to understanding the mechanisms that are responsible for surface water [waves](/source/Gravity_wave), lunar [tides](/source/Tide) and substantially contributes to weather patterns. Gravitational weight also has many important biological functions, helping to guide the growth of plants through the process of [gravitropism](/source/Gravitropism) and influencing the [circulation](/source/Circulatory_system) of fluids in [multicellular organisms](/source/Multicellular_organism).

## Characterization

Gravity is the word used to describe a [physical law](/source/Physical_law), a [fundamental physical interaction](/source/Fundamental_interaction) that derives primarily from [mass](/source/Mass), and the observed consequences of that interaction on objects. Gravity is the law that every object with mass attracts every other object in the universe in proportion to each mass and inversely proportional to the square of the distance between them. The force of gravity, F is written using the [gravitational constant](/source/Gravitational_constant), G, as[7] F = G m m ′ r 2 {\displaystyle F=G{\frac {mm'}{r^{2}}}} for two masses, m, and *m*′ separated by a distance r.

Gravity is considered to be one of four fundamental interactions. The [electromagnetic force](/source/Electromagnetic_force) law is similar to the force law for gravity: both depend upon the square of the inverse distance between objects in typical interactions. The ratio of gravitational attraction of two [electrons](/source/Electrons) to their electrical repulsion is 1 to 4.17×1042.[7] As a result, gravity can generally be neglected at the level of [subatomic particles](/source/Subatomic_particle).[8] Gravity becomes the most significant interaction between objects at the scale of astronomical bodies, and it determines the motion of [satellites](/source/Satellite), [planets](/source/Planet), [stars](/source/Star), [galaxies](/source/Galaxy), and even [light](/source/Electromagnetic_radiation). Gravity is also fundamental in another sense: the [inertial mass](/source/Inertial_mass) that appears in [Newton's second law](/source/Newton's_second_law) is the same as the [gravitational mass](/source/Gravitational_mass). This [equivalence principle](/source/Equivalence_principle) is a [scientific hypothesis](/source/Scientific_hypothesis) that has been tested experimentally to more than one part in a trillion.Navas, S.; et al. (August 2024). "Review of Particle Physics". *Physical Review D*. **110** (3). [doi](/source/Doi_(identifier)):[10.1103/PhysRevD.110.030001](https://doi.org/10.1103%2FPhysRevD.110.030001).

## History

Main article: [History of gravitational theory](/source/History_of_gravitational_theory)

### Ancient world

The nature and mechanism of gravity were explored by a wide range of ancient scholars. In [Ancient Greece](/source/Ancient_Greece), [Aristotle](/source/Aristotle) believed that each of the [classical elements](/source/Classical_elements) had a [natural place](/source/Aristotelian_physics#Natural_place) in the universe which it tends to move toward - earth at the center of the universe (the center of the Earth, which was known to be spherical); then water, air, fire, and aether in concentric shells from inner to outer.[9] He also thought that the speed of a falling object should increase with its weight, a conclusion that was later shown to be false.[10] While Aristotle's view was widely accepted throughout Ancient Greece, there were other thinkers such as [Plutarch](/source/Plutarch) who correctly predicted that the attraction of gravity was not unique to the Earth.[11]

Although he did not understand gravity as a force, the ancient Greek philosopher [Archimedes](/source/Archimedes) discovered the [center of gravity](/source/Center_of_gravity) of a triangle.[12] He postulated that if two equal weights did not have the same center of gravity, the center of gravity of the two weights together would be in the middle of the line that joins their centers of gravity.[13] Two centuries later, the Roman engineer and architect [Vitruvius](/source/Vitruvius) contended in his *[De architectura](/source/De_architectura)* that gravity is not dependent on a substance's weight but rather on its "nature".[14] In the 6th century CE, the [Byzantine](/source/Byzantine_Empire) Alexandrian scholar [John Philoponus](/source/John_Philoponus) proposed the theory of impetus, which modifies Aristotle's theory that "continuation of motion depends on continued action of a force" by incorporating a causative force that diminishes over time.[15]

In 628 CE, the [Indian](/source/India) mathematician and astronomer [Brahmagupta](/source/Brahmagupta) proposed the idea that gravity is an attractive force that draws objects to the Earth and used the term *[gurutvākarṣaṇ](https://en.wiktionary.org/wiki/%E0%A4%97%E0%A5%81%E0%A4%B0%E0%A5%81%E0%A4%A4%E0%A5%8D%E0%A4%B5%E0%A4%BE%E0%A4%95%E0%A4%B0%E0%A5%8D%E0%A4%B7%E0%A4%A3)* to describe it.[16]: 105[17][18]

In the ancient [Middle East](/source/Middle_East), gravity was a topic of fierce debate. The [Persian](/source/Persians) intellectual [Al-Biruni](/source/Al-Biruni) believed that the force of gravity was not unique to the Earth, and he correctly assumed that other [heavenly bodies](/source/Astronomical_object) should exert a gravitational attraction as well.[19] In contrast, [Al-Khazini](/source/Al-Khazini) held the same position as Aristotle that all matter in the [Universe](/source/Universe) is attracted to the center of the Earth.[20]

The [Leaning Tower of Pisa](/source/Leaning_Tower_of_Pisa), where according to legend Galileo performed an experiment about the speed of falling objects

### Scientific Revolution

Main article: [Scientific Revolution](/source/Scientific_Revolution)

In the mid-16th century, various European scientists experimentally disproved the [Aristotelian](/source/Aristotelian_physics) notion that heavier objects [fall](/source/Free_fall) at a faster rate.[21] In particular, the [Spanish](/source/Spanish_people) Dominican priest [Domingo de Soto](/source/Domingo_de_Soto) wrote in 1551 that bodies in free fall uniformly accelerate.[21] De Soto may have been influenced by earlier experiments conducted by other [Dominican](/source/Dominican_Order) priests in Italy, including those by [Benedetto Varchi](/source/Benedetto_Varchi), Francesco Beato, [Luca Ghini](/source/Luca_Ghini), and [Giovan Bellaso](/source/Giovan_Battista_Bellaso) which contradicted Aristotle's teachings on the fall of bodies.[21]

The mid-16th century Italian physicist [Giambattista Benedetti](/source/Giambattista_Benedetti) published papers claiming that, due to [specific gravity](/source/Relative_density), objects made of the same material but with different masses would fall at the same speed.[22] With the 1586 [Delft tower experiment](/source/Delft_tower_experiment), the [Flemish](/source/Flanders) physicist [Simon Stevin](/source/Simon_Stevin) observed that two cannonballs of differing sizes and weights fell at the same rate when dropped from a tower.[23]

In the late 16th century, [Galileo Galilei](/source/Galileo_Galilei)'s careful measurements of balls rolling down [inclines](/source/Inclined_plane) allowed him to firmly establish that gravitational acceleration is the same for all objects.[24][25]: 334 Galileo postulated that [air resistance](/source/Air_resistance) is the reason that objects with a low density and high [surface area](/source/Surface_area) fall more slowly in an atmosphere. In his 1638 work *[Two New Sciences](/source/Two_New_Sciences)*, Galileo proved that the distance traveled by a falling object is proportional to the [square](/source/Square_(algebra)) of the time elapsed. His method was a form of graphical numerical integration since concepts of algebra and calculus were unknown at the time.[26]: 4 This was later confirmed by Italian scientists [Jesuits](/source/Jesuits) [Grimaldi](/source/Francesco_Maria_Grimaldi) and [Riccioli](/source/Giovanni_Battista_Riccioli) between 1640 and 1650. They also calculated the magnitude of [the Earth's gravity](/source/Earth's_gravity) by measuring the oscillations of a pendulum.[27]

Galileo also broke with incorrect ideas of Aristotelian philosophy by regarding [inertia](/source/Inertia) as persistence of motion, not a tendency to come to rest. By considering that the laws of physics appear identical on a moving ship to those on land, Galileo developed the concepts of [reference frame](/source/Reference_frame) and the [principle of relativity](/source/Principle_of_relativity).[28]: 5 These concepts would become central to Newton's mechanics, only to be transformed in Einstein's theory of gravity, the general theory of relativity.[29]: 17

In last quarter of the 16th century [Tycho Brahe](/source/Tycho_Brahe) created accurate tools for [astrometry](/source/Astrometry), providing careful observations of the planets. His assistant and successor, [Johannes Kepler](/source/Johannes_Kepler) analyzed these data into three empirical laws of planetary motion. These laws were central to the development of a theory of gravity a hundred years later.[30] In his 1609 book [Astronomia nova](/source/Astronomia_nova) Kepler described gravity as a mutual attraction, claiming that if the Earth and Moon were not held apart by some force they would come together. He recognized that mechanical forces cause action, creating a kind of celestial machine. On the other hand Kepler viewed the force of the Sun on the planets as magnetic and acting tangential to their orbits and he assumed with Aristotle that inertia meant objects tend to come to rest.[31][32]: 846

In 1666, [Giovanni Alfonso Borelli](/source/Giovanni_Alfonso_Borelli) avoided the key problems that limited Kepler. By Borelli's time the concept of inertia had its modern meaning as the tendency of objects to remain in uniform motion and he viewed the Sun as just another heavenly body. Borelli developed the idea of mechanical equilibrium, a balance between inertia and gravity. Newton cited Borelli's influence on his theory.[32]: 848

In 1657, [Robert Hooke](/source/Robert_Hooke) published his *[Micrographia](/source/Micrographia)*, in which he hypothesized that the Moon must have its own gravity.[33]: 57 In a communication to the Royal Society in 1666 and his 1674 Gresham lecture, *An Attempt to prove the Annual Motion of the Earth*, Hooke took the important step of combining related hypothesis and then forming predictions based on the hypothesis.[34] He wrote:

I will explain a system of the world very different from any yet received. It is founded on the following positions. 1. That all the heavenly bodies have not only a gravitation of their parts to their own proper centre, but that they also mutually attract each other within their spheres of action. 2. That all bodies having a simple motion, will continue to move in a straight line, unless continually deflected from it by some extraneous force, causing them to describe a circle, an ellipse, or some other curve. 3. That this attraction is so much the greater as the bodies are nearer. As to the proportion in which those forces diminish by an increase of distance, I own I have not discovered it....[35][36]

Hooke was an important communicator who helped reformulate the scientific enterprise.[37] He was one of the first professional scientists and worked as the then-new [Royal Society](/source/Royal_Society)'s curator of experiments for 40 years.[38] However his valuable insights remained hypotheses and some of these were incorrect.[39] He was unable to develop a mathematical theory of gravity and work out the consequences.[32]: 853 For this he turned to Newton, writing him a letter in 1679, outlining a model of planetary motion in a void or vacuum due to attractive action at a distance. This letter likely turned Newton's thinking in a new direction leading to his revolutionary work on gravity.[37] When Newton reported his results in 1686, Hooke claimed the [inverse square law portion was his "notion"](/source/Newton%E2%80%93Hooke_priority_controversy_for_the_inverse_square_law).

### Newton's theory of gravitation

Main article: [Newton's law of universal gravitation](/source/Newton's_law_of_universal_gravitation)

English physicist and mathematician, Sir [Isaac Newton](/source/Isaac_Newton) (1642–1727)

Before 1684, scientists including [Christopher Wren](/source/Christopher_Wren), [Robert Hooke](/source/Robert_Hooke) and [Edmund Halley](/source/Edmund_Halley) determined that [Kepler's third law](/source/Kepler's_laws_of_planetary_motion), relating to planetary orbital periods, would prove the [inverse square law](/source/Inverse-square_law) if the orbits were circles. However the orbits were known to be ellipses. At Halley's suggestion, Newton tackled the problem and was able to prove that ellipses also proved the inverse square relation from Kepler's observations.[29]: 13 In 1684, [Isaac Newton](/source/Isaac_Newton) sent a manuscript to [Edmond Halley](/source/Edmond_Halley) titled *[De motu corporum in gyrum](/source/De_motu_corporum_in_gyrum) ('On the motion of bodies in an orbit')*, which provided a physical justification for Kepler's laws of planetary motion.[40] Halley was impressed by the manuscript and urged Newton to expand on it, and a few years later Newton published a groundbreaking book called *[Philosophiæ Naturalis Principia Mathematica](/source/Philosophi%C3%A6_Naturalis_Principia_Mathematica)* (*Mathematical Principles of Natural Philosophy*).

The revolutionary aspect of Newton's theory of gravity was the unification of Earth-bound observations of acceleration with celestial mechanics.[41]: 4 In his book, Newton described gravitation as a universal force, and claimed that it operated on objects "according to the quantity of solid matter which they contain and propagates on all sides to immense distances always at the inverse square of the distances".[42]: 546 This formulation had two important parts. First was [equating inertial mass and gravitational mass](/source/Equivalence_principle). Newton's 2nd law defines force via F = m a {\displaystyle F=ma} for inertial mass, his [law of gravitational](/source/Newton's_law_of_universal_gravitation) force uses the same mass. Newton did experiments with pendulums to verify this concept as best he could.[29]: 11

The second aspect of Newton's formulation was the inverse square of distance. This aspect was not new: the astronomer [Ismaël Bullialdus](/source/Isma%C3%ABl_Bullialdus) proposed it around 1640. Seeking proof, Newton made quantitative analysis around 1665, considering the period and distance of the Moon's orbit and considering the timing of objects falling on Earth. Newton did not publish these results at the time because he could not prove that the [Earth's gravity acts as if all its mass were concentrated at its center](/source/Shell_theorem). That proof took him twenty years.[29]: 13

Newton's *Principia* was well received by the scientific community, and his law of gravitation quickly spread across the European world. More than a century later, in 1821, his theory of gravitation rose to even greater prominence when it was used to predict the existence of [Neptune](/source/Neptune). In that year, the French astronomer [Alexis Bouvard](/source/Alexis_Bouvard) used this theory to create a table modeling the orbit of [Uranus](/source/Uranus), which was shown to differ significantly from the planet's actual trajectory. In order to explain this discrepancy, many astronomers speculated that there might be a large object beyond the orbit of Uranus which was disrupting its orbit. In 1846, the astronomers [John Couch Adams](/source/John_Couch_Adams) and [Urbain Le Verrier](/source/Urbain_Le_Verrier) independently used Newton's law to predict Neptune's location in the night sky, and the planet was discovered there within a day.[43][44]

Newton's formulation was later condensed into the inverse-square law: F = G m 1 m 2 r 2 , {\displaystyle F=G{\frac {m_{1}m_{2}}{r^{2}}},} where F is the force, *m*1 and *m*2 are the masses of the objects interacting, r is the distance between the centers of the masses and *G* is the [gravitational constant](/source/Gravitational_constant) 6.674×10−11 m3⋅kg−1⋅s−2.[45] While *G* is also called Newton's constant, Newton did not use this constant or formula, he only discussed proportionality. But this allowed him to come to an astounding conclusion we take for granted today: the gravity of the Earth on the Moon is the same as the gravity of the Earth on an apple: M earth ∝ a apple R radius of earth 2 = a moon R lunar orbit 2 {\displaystyle M_{\text{earth}}\propto a_{\text{apple}}R_{\text{radius of earth}}^{2}=a_{\text{moon}}R_{\text{lunar orbit}}^{2}} Using the values known at the time, Newton was able to verify this form of his law. The value of *G* was eventually [measured](/source/Cavendish_experiment) by [Henry Cavendish](/source/Henry_Cavendish) in 1797.[46]: 31

Newton's theory of gravity ran counter to a key idea of science, both then and now: forces should not rely on instantaneous [action at a distance](/source/Action_at_a_distance). Newton was well aware of this issue and his decision to continue anyway marked a shift in scientific thinking away from philosophically sound but empirically flawed models.[47]: 44 Scientists like [Gottfried Wilhelm Leibniz](/source/Gottfried_Wilhelm_Leibniz) complained about this aspect of the theory of gravity. [48]: 339 The issue was not resolved until Einstein's work on relativity in the 20th century.[7]

### Einstein's general relativity

Main article: [History of general relativity](/source/History_of_general_relativity)

General relativity G μ ν + Λ g μ ν = κ T μ ν {\displaystyle G_{\mu \nu }+\Lambda g_{\mu \nu }={\kappa }T_{\mu \nu }} Introduction History Timeline Tests Mathematical formulation Fundamental concepts Equivalence principle Special relativity World line Pseudo-Riemannian manifold Phenomena Kepler problem Gravitational lensing Gravitational redshift Gravitational time dilation Gravitational waves Frame-dragging Geodetic effect Event horizon Singularity Black hole Spacetime Spacetime diagrams Minkowski spacetime Metric tensor Equations Formalisms Equations Linearized gravity Einstein field equations Friedmann Geodesics Mathisson–Papapetrou–Dixon Hamilton–Jacobi–Einstein Raychaudhuri Teukolsky Formalisms ADM NP BSSN Post-Newtonian Advanced theory Kaluza–Klein theory Quantum gravity Quantum field theory in curved spacetime Solutions Schwarzschild (interior) Reissner–Nordström Einstein–Rosen waves Wormhole Gödel Kerr Kerr–Newman Kerr–Newman–de Sitter Kasner Kantowski-Sachs Lemaître–Tolman Wahlquist Taub–NUT Milne Robertson–Walker Oppenheimer–Snyder pp-wave van Stockum dust Hartle–Thorne Vaidya Peres De Sitter-Schwarzschild McVittie Weyl Scientists Einstein Lorentz Hilbert Poincaré Schwarzschild de Sitter Reissner Nordström Weyl Eddington Friedmann Milne Zwicky Lemaître Oppenheimer Gödel Wheeler Robertson Bardeen Walker Kerr Chandrasekhar Ehlers Penrose Hawking Raychaudhuri Taylor Hulse van Stockum Taub Newman Yau Thorne others Physics portal Category v t e

Eventually, astronomers noticed an eccentricity in the orbit of the planet [Mercury](/source/Mercury_(planet)) which could not be explained by Newton's theory: the [perihelion](/source/Perihelion) of the orbit was increasing by about 42.98 [arcseconds](/source/Arcseconds) per century. The most obvious explanation for this discrepancy was an as-yet-undiscovered celestial body, such as a planet orbiting the Sun even closer than Mercury, but all efforts to find such a body turned out to be fruitless. In 1915, [Albert Einstein](/source/Albert_Einstein) developed a theory of [general relativity](/source/General_relativity) which was able to accurately model Mercury's orbit.[49]

Einstein's theory brought two other ideas with independent histories into the physical theories of gravity: the [principle of relativity](/source/Principle_of_relativity) and [non-Euclidean geometry](/source/Non-Euclidean_geometry).

The principle of relativity, introduced by Galileo and used as a foundational principle by Newton, led to a long and fruitless search for a [luminiferous aether](/source/Luminiferous_aether) after [Maxwell's equations](/source/Maxwell's_equations) demonstrated that light propagated at a fixed speed independent of reference frame. In Newton's mechanics, velocities add: a cannon ball shot from a moving ship would travel with a trajectory which included the motion of the ship. Since light speed was fixed, it was assumed to travel in a fixed, absolute medium. Many experiments sought to reveal this medium but failed and in 1905 Einstein's [special relativity](/source/Special_relativity) theory showed the aether was not needed. Special relativity proposed that mechanics be reformulated to use the [Lorentz transformation](/source/Lorentz_transformation) already applicable to light rather than the [Galilean transformation](/source/Galilean_transformation) adopted by Newton. Special relativity, as in [special case](/source/Special_case), specifically did not cover gravity.[29]: 4

While relativity was associated with mechanics and thus gravity, the idea of altering geometry only joined the story of gravity once mechanics required the Lorentz transformations. [Geometry](/source/Geometry) was an [ancient science](/source/History_of_geometry) that gradually broke free of Euclidean limitations when [Carl Gauss](/source/Carl_Gauss) discovered in the 1800s that [surfaces in any number of dimensions](/source/Hypersurface) could be characterized by a [metric](/source/Metric_space), a distance measurement along the shortest path between two points that reduces to Euclidean distance at infinitesimal separation. Gauss' student [Bernhard Riemann](/source/Bernhard_Riemann) developed this into a complete geometry by 1854. These geometries are locally flat but have global [curvature](/source/Curvature).[29]: 4

In 1907, Einstein took his first step by using special relativity to create a new form of the [equivalence principle](/source/Equivalence_principle). The equivalence of inertial mass and gravitational mass was a known empirical law. The m in Newton's first law, F = m a {\displaystyle F=ma} , has the same value as the m in Newton's law of gravity on Earth, F = G M m / r 2 {\displaystyle F=GMm/r^{2}} . In what he later described as "the happiest thought of my life" Einstein realized this meant that in free-fall, an accelerated coordinate system exists with no local [gravitational field](/source/Gravitational_field).[50] Every description of gravity in any other coordinate system must transform to give no field in the free-fall case, a powerful [invariance](/source/Invariant_(physics)) constraint on all theories of gravity.[29]: 20

Einstein's description of gravity was accepted by the majority of physicists for two reasons. First, by 1910 his special relativity was accepted in German physics and was spreading to other countries. Second, his theory explained experimental results like the perihelion of Mercury and the bending of light around the Sun better than Newton's theory.[51]

In 1919, the British astrophysicist [Arthur Eddington](/source/Arthur_Eddington) was able to confirm the predicted deflection of light during [that year's solar eclipse](/source/Solar_eclipse_of_May_29%2C_1919).[52][53] Eddington measured starlight deflections twice those predicted by Newtonian corpuscular theory, in accordance with the predictions of general relativity. Although Eddington's analysis was later disputed, this experiment made Einstein famous almost overnight and caused general relativity to become widely accepted in the scientific community.[54]

In 1959, American physicists [Robert Pound](/source/Robert_Pound) and [Glen Rebka](/source/Glen_Rebka) performed [an experiment](/source/Pound%E2%80%93Rebka_experiment) in which they used [gamma rays](/source/Gamma_ray) to confirm the prediction of [gravitational time dilation](/source/Gravitational_time_dilation). By sending the rays down a 74-foot tower and measuring their frequency at the bottom, the scientists confirmed that light is [Doppler shifted](/source/Doppler_shift) as it moves towards a source of gravity. The observed shift also supports the idea that time runs more slowly in the presence of a gravitational field (many more wave crests pass in a given interval). If light moves outward from a strong source of gravity it will be observed with a [redshift](/source/Redshift).[55] The [time delay of light](/source/Time_delay_of_light) passing close to a massive object was first identified by [Irwin I. Shapiro](/source/Irwin_I._Shapiro) in 1964 in interplanetary spacecraft signals.[56]

In 1971, scientists made the first-ever discovery of a black hole, in the constellation [Cygnus](/source/Cygnus_(constellation)). The black hole was detected because it was emitting bursts of [x-rays](/source/X-rays) as it consumed a smaller star, and it came to be known as [Cygnus X-1](/source/Cygnus_X-1).[57] This discovery confirmed yet another prediction of general relativity, because Einstein's equations implied that light could not escape from a sufficiently large and compact object.[58]

[Frame dragging](/source/Frame_dragging), the idea that a rotating massive object should twist spacetime around it, was confirmed by [Gravity Probe B](/source/Gravity_Probe_B) results in 2011.[59][60] In 2015, the [LIGO](/source/LIGO) observatory detected faint [gravitational waves](/source/Gravitational_waves), the existence of which had been predicted by general relativity. Scientists believe that the waves emanated from a [black hole merger](/source/Black_hole_merger) that occurred 1.5 billion [light-years](/source/Light-years) away.[61]

## On Earth

An initially-stationary object that is allowed to fall freely under gravity drops a distance that is proportional to the square of the elapsed time. This image spans half a second and was captured at 20 flashes per second.

Main article: [Gravity of Earth](/source/Gravity_of_Earth)

Every planetary body (including the Earth) is surrounded by its own gravitational field, which can be conceptualized with Newtonian physics as exerting an attractive force on all objects. Assuming a spherically symmetrical planet, the strength of this field at any given point above the surface is proportional to the planetary body's mass and inversely proportional to the square of the distance from the center of the body.

If an object with comparable mass to that of the Earth were to fall towards it, then the corresponding acceleration of the Earth would be observable.

The strength of the gravitational field is numerically equal to the acceleration of objects under its influence.[62] The rate of acceleration of falling objects near the Earth's surface varies very slightly depending on latitude, surface features such as mountains and ridges, and perhaps unusually high or low sub-surface densities.[63] For purposes of weights and measures, a [standard gravity](/source/Standard_gravity) value is defined by the [International Bureau of Weights and Measures](/source/International_Bureau_of_Weights_and_Measures), under the [International System of Units](/source/International_System_of_Units) (SI).

The force of gravity experienced by objects on Earth's surface is the [vector sum](/source/Euclidean_vector) of two forces:[6] (a) The gravitational attraction in accordance with Newton's universal law of gravitation, and (b) the centrifugal force, which results from the choice of an earthbound, rotating frame of reference. The force of gravity is weakest at the equator because of the [centrifugal force](/source/Centrifugal_force) caused by the Earth's rotation and because points on the equator are farthest from the center of the Earth. The force of gravity varies with latitude, and the resultant acceleration increases from about 9.780 m/s2 at the Equator to about 9.832 m/s2 at the poles.[64][65]

### Gravity wave

Main article: [Gravity wave](/source/Gravity_wave)

Waves on oceans, lakes, and other bodies of water occur when the gravitational equilibrium at the surface of the water is disturbed by for example wind.[66] Similar effects occur in the [atmosphere](/source/Atmospheric_wave) where equilibrium is disturbed by thermal [weather fronts](/source/Weather_fronts) or mountain ranges.[67]

## Orbits

Main article: [Orbit](/source/Orbit)

[Planets](/source/Planets) orbit the [Sun](/source/Sun) in an [ellipse](/source/Ellipse) as a consequence of the law of gravity. Similarly the [Moon](/source/Moon) and artificial [satellites](/source/Satellites) orbit the Earth. Conceptually two objects in orbit are both falling off of the curve they would travel in if the force of gravity were not pulling them together. Since the force of gravity is universal, all planets attract each other with the most massive and closest pair have the most mutual affect. This means orbits are more complex than simple ellipses.[7]

## Astrophysics

### Stars and black holes

Main article: [Star formation](/source/Star_formation)

During star formation, gravitational attraction in a cloud of hydrogen gas competes with thermal gas pressure. As the gas density increases, the temperature rises, then the gas radiates energy, allowing additional gravitational condensation. If the mass of gas in the region is low, the process continues until a [brown dwarf](/source/Brown_dwarf) or [gas-giant planet](/source/Gas-giant_planet) is produced. If more mass is available, the additional gravitational energy allows the central region to reach pressures sufficient for [nuclear fusion](/source/Nuclear_fusion), forming a [star](/source/Star). In a star, again the gravitational attraction competes, with thermal and radiation pressure in [hydrostatic equilibrium](/source/Hydrostatic_equilibrium) until the star's atomic fuel runs out. The next phase depends upon the total mass of the star. Very low mass stars slowly cool as [white dwarf](/source/White_dwarf) stars with a small core balancing gravitational attraction with [electron degeneracy pressure](/source/Electron_degeneracy_pressure). Stars with masses similar to the Sun go through a [red giant](/source/Red_giant) phase before becoming white dwarf stars. Higher mass stars have complex core structures that burn helium and high atomic number elements ultimately producing an [iron](/source/Iron) core. As their fuel runs out, these stars become unstable producing a [supernova](/source/Supernova). The result can be a [neutron star](/source/Neutron_star) where gravitational attraction balances [neutron degeneracy pressure](/source/Neutron_degeneracy_pressure) or, for even higher masses, a [black hole](/source/Black_hole) where gravity operates alone with such intensity that even light cannot escape.[68]: 121

### Gravitational radiation

Main article: [Gravitational wave](/source/Gravitational_wave)

The [LIGO](/source/LIGO) Hanford Observatory located in Washington (state), United States, where gravitational waves were first observed in September 2015

General relativity predicts that energy can be transported out of a system through gravitational radiation also known as gravitational waves. The first indirect evidence for gravitational radiation was through measurements of the [Hulse–Taylor binary](/source/Hulse%E2%80%93Taylor_binary) in 1973. This system consists of a [pulsar](/source/Pulsar) and neutron star in orbit around one another. Its orbital period has decreased since its initial discovery due to a loss of energy, which is consistent for the amount of energy loss due to gravitational radiation. This research was awarded the [Nobel Prize in Physics](/source/Nobel_Prize_in_Physics) in 1993.[69]

The first direct evidence for gravitational radiation was measured on 14 September 2015 by the [LIGO](/source/LIGO) detectors. The gravitational waves emitted during the collision of two black holes 1.3 billion light years from Earth were measured.[70][71] This observation confirms the theoretical predictions of Einstein and others that such waves exist. It also opens the way for practical observation and understanding of the nature of gravity and events in the Universe including the Big Bang.[72] [Neutron star](/source/Neutron_star) and [black hole](/source/Black_hole) formation also create detectable amounts of gravitational radiation.[73] This research was awarded the Nobel Prize in Physics in 2017.[74]

### Dark matter

Main article: [Dark matter](/source/Dark_matter)

At the cosmological scale, gravity is a dominant player. About 5/6 of the total mass in the universe consists of dark matter which interacts through gravity but not through electromagnetic interactions. The gravitation of clumps of dark matter known as [dark matter halos](/source/Dark_matter_halo) attract hydrogen gas leading to stars and galaxies.[75]

### Gravitational lensing

Main article: [Gravitational lensing](/source/Gravitational_lensing)

[Einstein's Cross](/source/Einstein's_Cross), four images of the same distant [quasar](/source/Quasar) around a foreground galaxy due to gravitational lensing – a single quasar is actually hidden behind a massive foreground object (a galaxy in this case)

Gravity acts on light and matter equally, meaning that a sufficiently massive object could warp light around it and create a gravitational lens. This phenomenon was first confirmed by observation in 1979 using the 2.1 meter telescope at [Kitt Peak National Observatory](/source/Kitt_Peak_National_Observatory) in Arizona, which saw two mirror images of the same quasar whose light had been bent around the galaxy [YGKOW G1](/source/YGKOW_G1).[76][77] Many subsequent observations of gravitational lensing provide additional evidence for substantial amounts of dark matter around galaxies. Gravitational lenses do not focus like [eyeglass](/source/Eyeglass) lenses, but rather lead to annular shapes called [Einstein rings](/source/Einstein_rings).[46]: 370

### Speed of gravity

Main article: [Speed of gravity](/source/Speed_of_gravity)

In October 2017, the [LIGO](/source/LIGO) and [Virgo interferometer](/source/Virgo_interferometer) detectors received gravitational wave signals 2 seconds before [gamma ray](/source/Gamma_ray) satellites and optical telescopes seeing signals from the same direction, from a source about 130 million light-years away. This confirmed that the speed of gravitational waves was the same as the speed of light.[78]

### Anomalies and discrepancies

Not to be confused with [Gravity anomaly](/source/Gravity_anomaly).

There are some observations that are not adequately accounted for, which may point to the need for better theories of gravity or perhaps be explained in other ways.

Rotation curve of a typical spiral galaxy: predicted (A) and observed (B). The discrepancy between the curves is attributed to [dark matter](/source/Dark_matter).

- **[Galaxy rotation curves](/source/Galaxy_rotation_curve)**: Stars in galaxies follow a distribution of velocities where stars on the outskirts are moving faster than they should according to the observed distributions of luminous matter. Galaxies within [galaxy clusters](/source/Galaxy_groups_and_clusters) show a similar pattern. The pattern is considered strong evidence for [dark matter](/source/Dark_matter), which would interact through gravitation but not electromagnetically; various [modifications to Newtonian dynamics](/source/Modified_Newtonian_dynamics) have also been proposed.[79]

- **[Accelerated expansion](/source/Accelerated_expansion)**: The [expansion of the universe](/source/Expansion_of_the_universe) seems to be accelerating.[80] [Dark energy](/source/Dark_energy) has been proposed to explain this.[81]

- **[Flyby anomaly](/source/Flyby_anomaly)**: Various spacecraft have experienced greater acceleration than expected during [gravity assist](/source/Gravity_assist) maneuvers.[82] The [Pioneer anomaly](/source/Pioneer_anomaly) has been shown to be explained by thermal recoil due to the distant sun radiation on one side of the space craft.[83][84]

## Models

The physical models of gravity, like all physical models, are expressed mathematically. Physicists use several different models, depending on the problem to be solved or for the purpose of gaining physical intuition.[85]: 44

### Newtonian action-at-a-distance

[Newton's inverse square law](/source/Newton's_law_of_universal_gravitation) models gravity as a force F between two objects proportional to their mass, m: F 12 = G m 1 m 2 r 12 2 {\displaystyle F_{12}=G{\frac {m_{1}m_{2}}{{r_{12}}^{2}}}} This gravitational force causes the objects to accelerate towards each other unless balanced by other forces. The force is "nonlocal": it depends on the mass of an object at a distance.[85]: 44 Scientists from Newton onwards recognized that this [action at a distance](/source/Action_at_a_distance) does not explain the root cause of the force; this lack of a root cause was raised against Newton's theory at first.[86]: 339 Nevertheless the model explains a vast number of physical effects including cannon ball trajectories, tidal motion and planetary orbits.[85]: 4 Creating a theory independent of action at a distance requires combining the concept of [relativity](/source/Principle_of_relativity) with gravity, an enormously complex task using the Newtonian model.[85]: 48

### Gravitational field

Main article: [Gravitational field](/source/Gravitational_field)

A second equivalent approach to model gravity uses fields.[85]: 44 In physics, a field represents a physical phenomenon using a mathematical entity associated with each point in a space. Different field theories use different entities and concepts of space. For classical field theories of gravity, the entities can be vectors associated with points in a 3-dimensional space. Each vector gives the force experienced by an insignificantly small test mass at that point in space. The force vector at each point can be computed as the direction of the highest rate of change in the gravitational potential, a single number at each point in space. The three-dimensional map of the potential or of the gravitational field provides a visual representation of the effect of the gravitational effect of all surrounding objects.[*[dubious](https://en.wikipedia.org/wiki/Wikipedia:Accuracy_dispute#Disputed_statement) – [discuss](https://en.wikipedia.org/wiki/Talk:Gravity#Dubious)*] Field models are local: the field values on a sphere completely determine the effects of gravity with the sphere.[85]: 45

Fields are also used in general relativity, but rather than vectors over [Euclidean space](/source/Euclidean_space), the entities are [tensors](/source/Tensors) over [spacetime](/source/Spacetime). The [Einstein field equations](/source/Einstein_field_equations) relate the 10 independent values in the tensors to the distribution of mass and energy in space.[*[dubious](https://en.wikipedia.org/wiki/Wikipedia:Accuracy_dispute#Disputed_statement) – [discuss](https://en.wikipedia.org/wiki/Talk:Gravity#Dubious)*]

### Action principles

Main article: [Action principles](/source/Action_principles)

A third completely different way to derive a model of gravity is based on [action principles](/source/Action_principles). This formulation represents the effects of gravity on a system in a mathematically abstract way. The state of the system, for example the position and velocity of every particle, is expressed as a single mathematical entity. Each state has an associated energy property called the [Lagrangian](/source/Lagrangian_(mechanics)); the physically allowed changes to the state of the system minimize the value of this property. The path of the state is not a path in physical space, but rather in a high-dimensional state space: each point along the path corresponds to a different position and or velocity collectively for all particles in the system. This formulation does not express the forces or fields of the individual particles.[85]: 46 Modern theories of physics rely on these action principles.[87]: 396 The [Einstein field equation](/source/Einstein_field_equation) for gravitation can be derived from the [Einstein–Hilbert action](/source/Einstein%E2%80%93Hilbert_action).[87]: 388

## General relativity

See also: [Introduction to general relativity](/source/Introduction_to_general_relativity)

In [modern physics](/source/Modern_physics), general relativity is considered the most successful theory of gravitation.[88] Physicists continue to work to find [solutions](/source/Solutions_of_the_Einstein_field_equations) to the [Einstein field equations](/source/Einstein_field_equations) that form the basis of general relativity and continue to test the theory, finding excellent agreement in all cases.[89][90][91]: p.9

### Constraints

Any theory of gravity must conform to the requirements of special relativity and experimental observations. Newton's theory of gravity assumes [action at a distance](/source/Action_at_a_distance) and therefore cannot be reconciled with special relativity. The simplest generalization of Newton's approach would be a [scalar field](/source/Scalar_field) theory with the gravitational potential represented by a single number in a 4-dimensional spacetime. However, this type of theory fails to predict gravitational redshift or the deviation of light by matter and gives values for the precession of Mercury which are incorrect. A [vector field](/source/Vector_field) theory predicts negative energy gravitational waves so it also fails. Furthermore, no theory without curvature in spacetime can be consistent with special relativity. The simplest theory consistent with special relativity and the well-studied observations is general relativity.[92]

### General characteristics

Unlike Newton's formula with one parameter, *G*, force in general relativity is terms of 10 numbers formed in to a [metric tensor](/source/Metric_tensor).[29]: 70In general relativity the effects of gravitation are described in different ways in different frames of reference. In a free-falling or co-moving [coordinate system](/source/Coordinate_system), an object travels in a straight line. In other coordinate systems, the object accelerates and thus is seen to move under a force. The path in [spacetime](/source/Spacetime) (not 3D space) taken by a free-falling object is called a [geodesic](/source/Geodesic) and the length of that path as measured by time in the objects frame is the shortest (or rarely the longest) one. Consequently the effect of gravity can be described as curving spacetime. In a weak stationary gravitational field, general relativity reduces to Newton's equations. The corrections introduced by general relativity on Earth are on the order of 1 part in a billion.[29]: 77

### Einstein field equations

Main article: [Einstein field equations](/source/Einstein_field_equations)

The Einstein field equations are a [system](/source/System_of_equations) of 10 [partial differential equations](/source/Partial_differential_equation) which describe how matter affects the curvature of spacetime. The system may be expressed in the form G μ ν + Λ g μ ν = κ T μ ν , {\displaystyle G_{\mu \nu }+\Lambda g_{\mu \nu }=\kappa T_{\mu \nu },} where Gμν is the [Einstein tensor](/source/Einstein_tensor), gμν is the [metric tensor](/source/Metric_tensor_(general_relativity)), Tμν is the [stress–energy tensor](/source/Stress%E2%80%93energy_tensor), Λ is the [cosmological constant](/source/Cosmological_constant), G {\displaystyle G} is the Newtonian constant of gravitation and c {\displaystyle c} is the [speed of light](/source/Speed_of_light).[93] The constant κ = 8 π G c 4 {\displaystyle \kappa ={\frac {8\pi G}{c^{4}}}} is referred to as the Einstein gravitational constant.[94]

### Solutions

Main article: [Solutions of the Einstein field equations](/source/Solutions_of_the_Einstein_field_equations)

The non-linear second-order Einstein field equations are extremely complex and have been solved in only a few special cases.[95] These cases however have been transformational in our understanding of the cosmos. Several solutions are the basis for understanding [black holes](/source/Black_holes) and for our modern model of the evolution of the universe since the [Big Bang](/source/Big_Bang).[41]: 227

### Tests of general relativity

Main article: [Tests of general relativity](/source/Tests_of_general_relativity)

The 1919 [total solar eclipse](/source/Total_solar_eclipse) provided one of the first opportunities to test the predictions of general relativity.

Testing the predictions of general relativity has historically been difficult, because they are almost identical to the predictions of Newtonian gravity for small energies and masses.[96] A wide range of experiments provided support of general relativity.[91]: 1–9[97][98][99][100] Today, Einstein's theory of relativity is used for all gravitational calculations where absolute precision is desired, although Newton's inverse-square law is accurate enough for virtually all ordinary calculations.[91]: 79[101]

### Gravity and quantum mechanics

Main articles: [Graviton](/source/Graviton) and [Quantum gravity](/source/Quantum_gravity)

Despite its success in predicting the effects of gravity at large scales, general relativity is ultimately incompatible with [quantum mechanics](/source/Quantum_mechanics). This is because general relativity describes gravity as a smooth, continuous distortion of spacetime, while quantum mechanics holds that all forces arise from the exchange of discrete particles known as [quanta](/source/Quantum). This contradiction is especially vexing to physicists because the other three fundamental forces (strong force, weak force and electromagnetism) were reconciled with a quantum framework decades ago.[102] As a result, researchers have begun to search for a theory that could unite both gravity and quantum mechanics under a more general framework.[103]

One path is to describe gravity in the framework of [quantum field theory](/source/Quantum_field_theory) (QFT), which has been successful to accurately describe the other [fundamental interactions](/source/Fundamental_interaction). The electromagnetic force arises from an exchange of virtual [photons](/source/Photon), where the QFT description of gravity is that there is an exchange of [virtual](/source/Virtual_particle) [gravitons](/source/Graviton).[104][105] This description reproduces general relativity in the [classical limit](/source/Classical_limit). However, this approach fails at short distances of the order of the [Planck length](/source/Planck_length),[106] where a more complete theory of [quantum gravity](/source/Quantum_gravity) (or a new approach to quantum mechanics) is required.

### Alternative theories

Main article: [Alternatives to general relativity](/source/Alternatives_to_general_relativity)

General relativity has withstood many [tests](/source/Tests_of_general_relativity) over a large range of mass and size scales.[107][108] When applied to interpret astronomical observations, cosmological models based on general relativity introduce two components to the universe,[109] [dark matter](/source/Dark_matter)[110] and [dark energy](/source/Dark_energy),[111] the nature of which is currently an [unsolved problem in physics](/source/List_of_unsolved_problems_in_physics#Cosmology_and_general_relativity). The many successful, high precision predictions of the [standard model of cosmology](/source/Lambda-CDM_model) has led astrophysicists to conclude it and thus general relativity will be the basis for future progress.[112][113] However, dark matter is not supported by the [Standard Model of particle physics](/source/Standard_Model_of_particle_physics), physical models for dark energy do not match cosmological data, and some cosmological observations are inconsistent.[113] These issues have led to the study of alternative theories of gravity.[114]

## See also

- [Anti-gravity](/source/Anti-gravity) – Physical and science fiction concept

- [Artificial gravity](/source/Artificial_gravity) – Use of circular rotational force to mimic gravity

- [Equations for a falling body](/source/Equations_for_a_falling_body) – Mathematical description of a body in free fall

- [Escape velocity](/source/Escape_velocity) – Concept in celestial mechanics

- [Atmospheric escape](/source/Atmospheric_escape) – Loss of planetary atmospheric gases to outer space

- [Gauss's law for gravity](/source/Gauss's_law_for_gravity) – Restatement of Newton's law of universal gravitation

- [Gravitational potential](/source/Gravitational_potential) – Fundamental study of potential theory

- [Gravitational biology](/source/Gravitational_biology) – Effect of gravity on living organisms

- [Newton's laws of motion](/source/Newton's_laws_of_motion) – Laws in physics about force and motion

- [Standard gravitational parameter](/source/Standard_gravitational_parameter) – Concept in celestial mechanics

- [Weightlessness](/source/Weightlessness) – Absence of the sensation of weight

## References

1. **[^](#cite_ref-1)** ["dict.cc dictionary :: gravitas :: English-Latin translation"](https://browse.dict.cc/latin-english/gravitas.html). [Archived](https://web.archive.org/web/20210813203625/https://browse.dict.cc/latin-english/gravitas.html) from the original on 13 August 2021. Retrieved 11 September 2018.

1. **[^](#cite_ref-2)** Braibant, Sylvie; Giacomelli, Giorgio; Spurio, Maurizio (2011). [*Particles and Fundamental Interactions: An Introduction to Particle Physics*](https://books.google.com/books?id=0Pp-f0G9_9sC) (illustrated ed.). Springer Science & Business Media. p. 109. [ISBN](/source/ISBN_(identifier)) [978-94-007-2463-1](https://en.wikipedia.org/wiki/Special:BookSources/978-94-007-2463-1). [Extract of page 109](https://books.google.com/books?id=0Pp-f0G9_9sC&pg=PA109)

1. **[^](#cite_ref-3)** ["HubbleSite: Black Holes: Gravity's Relentless Pull"](http://hubblesite.org/explore_astronomy/black_holes/home.html). *hubblesite.org*. [Archived](https://web.archive.org/web/20181226185228/http://hubblesite.org/explore_astronomy/black_holes/home.html) from the original on 26 December 2018. Retrieved 7 October 2016.

1. **[^](#cite_ref-NYT-20221010_4-0)** [Overbye, Dennis](/source/Dennis_Overbye) (10 October 2022). ["Black Holes May Hide a Mind-Bending Secret About Our Universe – Take gravity, add quantum mechanics, stir. What do you get? Just maybe, a holographic cosmos"](https://www.nytimes.com/2022/10/10/science/black-holes-cosmology-hologram.html). *[The New York Times](/source/The_New_York_Times)*. [Archived](https://web.archive.org/web/20221116151210/https://www.nytimes.com/2022/10/10/science/black-holes-cosmology-hologram.html) from the original on 16 November 2022. Retrieved 10 October 2022.

1. **[^](#cite_ref-5)** Cartwright, Jon (17 May 2025). "Defying gravity". *New Scientist*. pp. 30–33.

1. ^ [***a***](#cite_ref-HWM_6-0) [***b***](#cite_ref-HWM_6-1) Hofmann-Wellenhof, B.; Moritz, H. (2006). *Physical Geodesy* (2nd ed.). Springer. [ISBN](/source/ISBN_(identifier)) [978-3-211-33544-4](https://en.wikipedia.org/wiki/Special:BookSources/978-3-211-33544-4). § 2.1: "The total force acting on a body at rest on the earth's surface is the resultant of gravitational force and the centrifugal force of the earth's rotation and is called gravity.

1. ^ [***a***](#cite_ref-Feynman-7_7-0) [***b***](#cite_ref-Feynman-7_7-1) [***c***](#cite_ref-Feynman-7_7-2) [***d***](#cite_ref-Feynman-7_7-3) Feynman, Richard P.; Leighton, Robert B.; Sands, Matthew L. (2006). ["The Theory of Gravitation"](https://www.feynmanlectures.caltech.edu/I_07.html). *The Feynman lectures on physics* (Definitive ed.). San Francisco, Calif.: Pearson Addison Wesley. [ISBN](/source/ISBN_(identifier)) [978-0-8053-9045-2](https://en.wikipedia.org/wiki/Special:BookSources/978-0-8053-9045-2).

1. **[^](#cite_ref-8)** Krebs, Robert E. (1999). [*Scientific Development and Misconceptions Through the Ages: A Reference Guide*](https://archive.org/details/scientificdevelo0000kreb) (illustrated ed.). Greenwood Publishing Group. p. [133](https://archive.org/details/scientificdevelo0000kreb/page/133). [ISBN](/source/ISBN_(identifier)) [978-0-313-30226-8](https://en.wikipedia.org/wiki/Special:BookSources/978-0-313-30226-8).

1. **[^](#cite_ref-9)** *[De Caelo](/source/De_Caelo)* II. 13-14.

1. **[^](#cite_ref-10)** Cappi, Alberto. ["The concept of gravity before Newton"](http://www.cultureandcosmos.org/pdfs/16/Cappi_INSAPVII_Gravity_before_Newton.pdf) (PDF). *Culture and Cosmos*. [Archived](https://ghostarchive.org/archive/20221009/http://www.cultureandcosmos.org/pdfs/16/Cappi_INSAPVII_Gravity_before_Newton.pdf) (PDF) from the original on 9 October 2022.

1. **[^](#cite_ref-11)** Bakker, Frederik; Palmerino, Carla Rita (June 2020). "Motion to the Center or Motion to the Whole? Plutarch's Views on Gravity and Their Influence on Galileo". *Isis*. **111** (2): 217–238. [doi](/source/Doi_(identifier)):[10.1086/709138](https://doi.org/10.1086%2F709138). [hdl](/source/Hdl_(identifier)):[2066/219256](https://hdl.handle.net/2066%2F219256). [JSTOR](/source/JSTOR_(identifier)) [48779301](https://www.jstor.org/stable/48779301).

1. **[^](#cite_ref-12)** Neitz, Reviel; Noel, William (13 October 2011). [*The Archimedes Codex: Revealing The Secrets of the World's Greatest Palimpsest*](https://books.google.com/books?id=ZC1MOaAkKnsC&pg=PT125). Hachette UK. p. 125. [ISBN](/source/ISBN_(identifier)) [978-1-78022-198-4](https://en.wikipedia.org/wiki/Special:BookSources/978-1-78022-198-4). [Archived](https://web.archive.org/web/20200107004958/https://books.google.com/books?id=ZC1MOaAkKnsC&pg=PT125) from the original on 7 January 2020. Retrieved 10 April 2019.

1. **[^](#cite_ref-13)** Tuplin, CJ; Wolpert, Lewis (2002). [*Science and Mathematics in Ancient Greek Culture*](https://books.google.com/books?id=ajGkvOo0egwC&pg=PR11). Hachette UK. p. xi. [ISBN](/source/ISBN_(identifier)) [978-0-19-815248-4](https://en.wikipedia.org/wiki/Special:BookSources/978-0-19-815248-4). [Archived](https://web.archive.org/web/20200117170945/https://books.google.com/books?id=ajGkvOo0egwC&pg=PR11) from the original on 17 January 2020. Retrieved 10 April 2019.

1. **[^](#cite_ref-14)** [Vitruvius, Marcus Pollio](/source/Marcus_Vitruvius_Pollio) (1914). ["Chapter VII - Nature Colours"](https://web.archive.org/web/20161013193438/http://www.gutenberg.org/files/20239/20239-h/29239-h.htm#Page_215). In Alfred A. Howard (ed.). *De Architectura libri decem* [*Ten Books on Architecture*]. Herbert Langford Warren, Nelson Robinson (illus), Morris Hicky Morgan. Harvard University, Cambridge: Harvard University Press. p. 215. Archived from [the original](http://www.gutenberg.org/files/20239/20239-h/29239-h.htm#Page_215) on 13 October 2016. Retrieved 10 April 2019.

1. **[^](#cite_ref-15)** Philoponus' term for impetus is "ἑνέργεια ἀσώματος κινητική" ("incorporeal motive *[enérgeia](/source/Potentiality_and_actuality)*"); see *[CAG](/source/Commentaria_in_Aristotelem_Graeca)* XVII, [*Ioannis Philoponi in Aristotelis Physicorum Libros Quinque Posteriores Commentaria*](https://books.google.com/books?id=dVcqvVDiNVUC) [Archived](https://web.archive.org/web/20231222224140/https://books.google.com/books?id=dVcqvVDiNVUC) 22 December 2023 at the [Wayback Machine](/source/Wayback_Machine), [Walter de Gruyter](/source/Walter_de_Gruyter), 1888, p. 642: "λέγω δὴ ὅτι ἑνέργειά τις ἀσώματος κινητικὴ ἑνδίδοται ὑπὸ τοῦ ῥιπτοῦντος τῷ ῥιπτουμένῳ [I say that impetus (incorporeal motive energy) is transferred from the thrower to the thrown]."

1. **[^](#cite_ref-16)** Pickover, Clifford (16 April 2008). [*Archimedes to Hawking: Laws of Science and the Great Minds Behind Them*](https://books.google.com/books?id=SQXcpvjcJBUC&pg=PA105). Oxford University Press. [ISBN](/source/ISBN_(identifier)) [978-0-19-979268-9](https://en.wikipedia.org/wiki/Special:BookSources/978-0-19-979268-9). [Archived](https://web.archive.org/web/20170118060420/https://books.google.com/books?id=SQXcpvjcJBUC) from the original on 18 January 2017. Retrieved 29 August 2017.

1. **[^](#cite_ref-17)** Bose, Mainak Kumar (1988). [*Late classical India*](https://books.google.com/books?id=nbItAAAAMAAJ&q=gravity). A. Mukherjee & Co. [Archived](https://web.archive.org/web/20210813203602/https://books.google.com/books?id=nbItAAAAMAAJ&q=gravity) from the original on 13 August 2021. Retrieved 28 July 2021.

1. **[^](#cite_ref-18)** Sen, Amartya (2005). *The Argumentative Indian*. Allen Lane. p. 29. [ISBN](/source/ISBN_(identifier)) [978-0-7139-9687-6](https://en.wikipedia.org/wiki/Special:BookSources/978-0-7139-9687-6).

1. **[^](#cite_ref-19)** Starr, S. Frederick (2015). [*Lost Enlightenment: Central Asia's Golden Age from the Arab Conquest to Tamerlane*](https://books.google.com/books?id=hWyYDwAAQBAJ&pg=PA260). Princeton University Press. p. 260. [ISBN](/source/ISBN_(identifier)) [978-0-691-16585-1](https://en.wikipedia.org/wiki/Special:BookSources/978-0-691-16585-1).

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1. ^ [***a***](#cite_ref-Wallace-2018_21-0) [***b***](#cite_ref-Wallace-2018_21-1) [***c***](#cite_ref-Wallace-2018_21-2) Wallace, William A. (2018) [2004]. [*Domingo de Soto and the Early Galileo: Essays on Intellectual History*](https://books.google.com/books?id=8GxQDwAAQBAJ&pg=PR21). Abingdon, UK: [Routledge](/source/Routledge). pp. 119, 121–22. [ISBN](/source/ISBN_(identifier)) [978-1-351-15959-3](https://en.wikipedia.org/wiki/Special:BookSources/978-1-351-15959-3). [Archived](https://web.archive.org/web/20210616043300/https://books.google.com/books?id=8GxQDwAAQBAJ&pg=PR21) from the original on 16 June 2021. Retrieved 4 August 2021.

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1. **[^](#cite_ref-PhysRev2017_73-0)** Abbott, B. P.; et al. ([LIGO Scientific Collaboration](/source/LIGO_Scientific_Collaboration) & [Virgo Collaboration](/source/Virgo_interferometer)) (October 2017). ["GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral"](https://doi.org/10.1103%2FPhysRevLett.119.161101). *[Physical Review Letters](/source/Physical_Review_Letters)*. **119** (16) 161101. [arXiv](/source/ArXiv_(identifier)):[1710.05832](https://arxiv.org/abs/1710.05832). [Bibcode](/source/Bibcode_(identifier)):[2017PhRvL.119p1101A](https://ui.adsabs.harvard.edu/abs/2017PhRvL.119p1101A). [doi](/source/Doi_(identifier)):[10.1103/PhysRevLett.119.161101](https://doi.org/10.1103%2FPhysRevLett.119.161101). [PMID](/source/PMID_(identifier)) [29099225](https://pubmed.ncbi.nlm.nih.gov/29099225).

1. **[^](#cite_ref-74)** Devlin, Hanna (3 October 2017). ["Nobel prize in physics awarded for discovery of gravitational waves"](https://www.theguardian.com/science/2017/oct/03/nobel-prize-physics-discovery-gravitational-waves-ligo). *the Guardian*. [Archived](https://web.archive.org/web/20171003102211/https://www.theguardian.com/science/2017/oct/03/nobel-prize-physics-discovery-gravitational-waves-ligo) from the original on 3 October 2017. Retrieved 3 October 2017.

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1. **[^](#cite_ref-76)** Kar, Subal (2022). [*Physics and Astrophysics: Glimpses of the Progress*](https://books.google.com/books?id=IWFkEAAAQBAJ) (illustrated ed.). CRC Press. p. 106. [ISBN](/source/ISBN_(identifier)) [978-1-000-55926-2](https://en.wikipedia.org/wiki/Special:BookSources/978-1-000-55926-2). [Extract of page 106](https://books.google.com/books?id=IWFkEAAAQBAJ&pg=PT106).

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1. ^ [***a***](#cite_ref-FeynmanLaw_85-0) [***b***](#cite_ref-FeynmanLaw_85-1) [***c***](#cite_ref-FeynmanLaw_85-2) [***d***](#cite_ref-FeynmanLaw_85-3) [***e***](#cite_ref-FeynmanLaw_85-4) [***f***](#cite_ref-FeynmanLaw_85-5) [***g***](#cite_ref-FeynmanLaw_85-6) Feynman, Richard P. (1990). *The character of physical law* (16. pr ed.). Cambridge, Mass.: MIT Press. [ISBN](/source/ISBN_(identifier)) [978-0-262-56003-0](https://en.wikipedia.org/wiki/Special:BookSources/978-0-262-56003-0).

1. **[^](#cite_ref-86)** Hesse, Mary B. (1955). "Action at a Distance in Classical Physics". *Isis*. **46** (4): 337–353. [doi](/source/Doi_(identifier)):[10.1086/348429](https://doi.org/10.1086%2F348429). [JSTOR](/source/JSTOR_(identifier)) [227576](https://www.jstor.org/stable/227576).

1. ^ [***a***](#cite_ref-ZeeEnstein_87-0) [***b***](#cite_ref-ZeeEnstein_87-1) Zee, Anthony (2013). *Einstein Gravity in a Nutshell*. In a Nutshell Series (1st ed.). Princeton: Princeton University Press. [ISBN](/source/ISBN_(identifier)) [978-0-691-14558-7](https://en.wikipedia.org/wiki/Special:BookSources/978-0-691-14558-7).

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1. **[^](#cite_ref-Lea_90-0)** Lea, Robert (15 September 2022). ["Einstein's greatest theory just passed its most rigorous test yet"](https://www.scientificamerican.com/article/einsteins-greatest-theory-just-passed-its-most-rigorous-test-yet/). *Scientific American*. Springer Nature America, Inc. Retrieved 11 August 2024.

1. ^ [***a***](#cite_ref-Will_91-0) [***b***](#cite_ref-Will_91-1) [***c***](#cite_ref-Will_91-2) Will, Clifford M. (2018). [*Theory and Experiment in Gravitational Physics*](https://books.google.com/books?id=gf1uDwAAQBAJ). Cambridge Univ. Press. [ISBN](/source/ISBN_(identifier)) [978-1-107-11744-0](https://en.wikipedia.org/wiki/Special:BookSources/978-1-107-11744-0).

1. **[^](#cite_ref-92)** Debono, Ivan; Smoot, George (28 September 2016). ["General Relativity and Cosmology: Unsolved Questions and Future Directions"](https://doi.org/10.3390%2Funiverse2040023). *Universe*. **2** (4): 23. [arXiv](/source/ArXiv_(identifier)):[1609.09781](https://arxiv.org/abs/1609.09781). [Bibcode](/source/Bibcode_(identifier)):[2016Univ....2...23D](https://ui.adsabs.harvard.edu/abs/2016Univ....2...23D). [doi](/source/Doi_(identifier)):[10.3390/universe2040023](https://doi.org/10.3390%2Funiverse2040023).

1. **[^](#cite_ref-93)** ["Einstein Field Equations (General Relativity)"](https://warwick.ac.uk/fac/sci/physics/intranet/pendulum/generalrelativity/). *University of Warwick*. [Archived](https://web.archive.org/web/20220525140036/https://warwick.ac.uk/fac/sci/physics/intranet/pendulum/generalrelativity/) from the original on 25 May 2022. Retrieved 24 May 2022.

1. **[^](#cite_ref-94)** ["How to understand Einstein's equation for general relativity"](https://bigthink.com/starts-with-a-bang/einstein-general-theory-relativity-equation/). *Big Think*. 15 September 2021. [Archived](https://web.archive.org/web/20220526023430/https://bigthink.com/starts-with-a-bang/einstein-general-theory-relativity-equation/) from the original on 26 May 2022. Retrieved 24 May 2022.

1. **[^](#cite_ref-95)** Siegel, Ethan. ["This Is Why Scientists Will Never Exactly Solve General Relativity"](https://www.forbes.com/sites/startswithabang/2019/12/04/this-is-why-scientists-will-never-exactly-solve-general-relativity/). *Forbes*. [Archived](https://web.archive.org/web/20220527212804/https://www.forbes.com/sites/startswithabang/2019/12/04/this-is-why-scientists-will-never-exactly-solve-general-relativity/) from the original on 27 May 2022. Retrieved 27 May 2022.

1. **[^](#cite_ref-NASA-2022_96-0)** ["Testing General Relativity"](https://asd.gsfc.nasa.gov/blueshift/index.php/2015/11/27/testing-general-relativity/). *NASA Blueshift*. [Archived](https://web.archive.org/web/20220516115115/https://asd.gsfc.nasa.gov/blueshift/index.php/2015/11/27/testing-general-relativity/) from the original on 16 May 2022. Retrieved 29 May 2022.

1. **[^](#cite_ref-97)** Lindley, David (12 July 2005). ["The Weight of Light"](https://physics.aps.org/story/v16/st1). *Physics*. **16**. [Archived](https://web.archive.org/web/20220525201415/https://physics.aps.org/story/v16/st1) from the original on 25 May 2022. Retrieved 22 May 2022.

1. **[^](#cite_ref-98)** ["Hafele-Keating Experiment"](http://hyperphysics.phy-astr.gsu.edu/hbase/Relativ/airtim.html). *hyperphysics.phy-astr.gsu.edu*. [Archived](https://web.archive.org/web/20170418005731/http://hyperphysics.phy-astr.gsu.edu/hbase/Relativ/airtim.html) from the original on 18 April 2017. Retrieved 22 May 2022.

1. **[^](#cite_ref-99)** ["How the 1919 Solar Eclipse Made Einstein the World's Most Famous Scientist"](https://www.discovermagazine.com/the-sciences/how-the-1919-solar-eclipse-made-einstein-the-worlds-most-famous-scientist). *Discover Magazine*. 24 May 2019. [Archived](https://web.archive.org/web/20220522141013/https://www.discovermagazine.com/the-sciences/how-the-1919-solar-eclipse-made-einstein-the-worlds-most-famous-scientist) from the original on 22 May 2022. Retrieved 22 May 2022.

1. **[^](#cite_ref-100)** Cho, Adrian (4 May 2011). ["At Long Last, Gravity Probe B Satellite Proves Einstein Right"](https://www.science.org/content/article/long-last-gravity-probe-b-satellite-proves-einstein-right). *Science*. [Archived](https://web.archive.org/web/20220522141013/https://www.science.org/content/article/long-last-gravity-probe-b-satellite-proves-einstein-right) from the original on 22 May 2022. Retrieved 22 May 2022.

1. **[^](#cite_ref-Hassani_101-0)** Hassani, Sadri (2010). [*From Atoms to Galaxies: A conceptual physics approach to scientific awareness*](https://books.google.com/books?id=oypZ_a9pqdsC&pg=PA131). CRC Press. p. 131. [ISBN](/source/ISBN_(identifier)) [978-1-4398-0850-4](https://en.wikipedia.org/wiki/Special:BookSources/978-1-4398-0850-4).

1. **[^](#cite_ref-102)** ["Gravity Probe B – Special & General Relativity Questions and Answers"](https://einstein.stanford.edu/content/relativity/a11758.html#:~:text=Quantum%20mechanics%20is%20incompatible%20with,exchange%20of%20well-defined%20quanta.). *einstein.stanford.edu*. [Archived](https://web.archive.org/web/20220606161408/https://einstein.stanford.edu/content/relativity/a11758.html#:~:text=Quantum%20mechanics%20is%20incompatible%20with,exchange%20of%20well-defined%20quanta.) from the original on 6 June 2022. Retrieved 1 August 2022.

1. **[^](#cite_ref-103)** Huggett, Nick; Matsubara, Keizo; Wüthrich, Christian (2020). *Beyond Spacetime: The Foundations of Quantum Gravity*. [Cambridge University Press](/source/Cambridge_University_Press). p. 6. [ISBN](/source/ISBN_(identifier)) [978-1-108-65570-5](https://en.wikipedia.org/wiki/Special:BookSources/978-1-108-65570-5).

1. **[^](#cite_ref-104)** Feynman, R. P.; Morinigo, F. B.; Wagner, W. G.; Hatfield, B. (1995). [*Feynman lectures on gravitation*](https://archive.org/details/feynmanlectureso0000feyn_g4q1). Addison-Wesley. [ISBN](/source/ISBN_(identifier)) [978-0-201-62734-3](https://en.wikipedia.org/wiki/Special:BookSources/978-0-201-62734-3).

1. **[^](#cite_ref-105)** Zee, A. (2003). *Quantum Field Theory in a Nutshell*. Princeton University Press. [ISBN](/source/ISBN_(identifier)) [978-0-691-01019-9](https://en.wikipedia.org/wiki/Special:BookSources/978-0-691-01019-9).

1. **[^](#cite_ref-Randall,_Lisa_2005_106-0)** Randall, Lisa (2005). [*Warped Passages: Unraveling the Universe's Hidden Dimensions*](https://archive.org/details/warpedpassagesun00rand_1). Ecco. [ISBN](/source/ISBN_(identifier)) [978-0-06-053108-9](https://en.wikipedia.org/wiki/Special:BookSources/978-0-06-053108-9).

1. **[^](#cite_ref-WillReview2014_107-0)** Will, Clifford M. (December 2014). ["The Confrontation between General Relativity and Experiment"](https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5255900). *Living Reviews in Relativity*. **17** (1) 4. [arXiv](/source/ArXiv_(identifier)):[1403.7377](https://arxiv.org/abs/1403.7377). [Bibcode](/source/Bibcode_(identifier)):[2014LRR....17....4W](https://ui.adsabs.harvard.edu/abs/2014LRR....17....4W). [doi](/source/Doi_(identifier)):[10.12942/lrr-2014-4](https://doi.org/10.12942%2Flrr-2014-4). [PMC](/source/PMC_(identifier)) [5255900](https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5255900). [PMID](/source/PMID_(identifier)) [28179848](https://pubmed.ncbi.nlm.nih.gov/28179848).

1. **[^](#cite_ref-108)** Asmodelle, E. (2017). "Tests of General Relativity: A Review". [arXiv](/source/ArXiv_(identifier)):[1705.04397v1](https://arxiv.org/abs/1705.04397v1) [[physics.class-ph](https://arxiv.org/archive/physics.class-ph)].

1. **[^](#cite_ref-k889_109-0)** Ryden, Barbara Sue (2017). *Introduction to cosmology*. Cambridge: Cambridge University Press. [ISBN](/source/ISBN_(identifier)) [978-1-316-65108-7](https://en.wikipedia.org/wiki/Special:BookSources/978-1-316-65108-7).

1. **[^](#cite_ref-dm_110-0)** Garrett, Katherine; Duda, Gintaras (2011). ["Dark Matter: A Primer"](https://doi.org/10.1155%2F2011%2F968283). *Advances in Astronomy*. **2011**: 1–22. [arXiv](/source/ArXiv_(identifier)):[1006.2483](https://arxiv.org/abs/1006.2483). [Bibcode](/source/Bibcode_(identifier)):[2011AdAst2011E...8G](https://ui.adsabs.harvard.edu/abs/2011AdAst2011E...8G). [doi](/source/Doi_(identifier)):[10.1155/2011/968283](https://doi.org/10.1155%2F2011%2F968283).

1. **[^](#cite_ref-de_111-0)** Li, Miao; Li, Xiao-Dong; Wang, Shuang; Wang, Yi (December 2013). "Dark energy: A brief review". *Frontiers of Physics*. **8** (6): 828–846. [arXiv](/source/ArXiv_(identifier)):[1209.0922](https://arxiv.org/abs/1209.0922). [Bibcode](/source/Bibcode_(identifier)):[2013FrPhy...8..828L](https://ui.adsabs.harvard.edu/abs/2013FrPhy...8..828L). [doi](/source/Doi_(identifier)):[10.1007/s11467-013-0300-5](https://doi.org/10.1007%2Fs11467-013-0300-5).

1. **[^](#cite_ref-Turner-2022_112-0)** Turner, Michael S. (26 September 2022). "The Road to Precision Cosmology". *Annual Review of Nuclear and Particle Science*. **72** (1): 1–35. [arXiv](/source/ArXiv_(identifier)):[2201.04741](https://arxiv.org/abs/2201.04741). [Bibcode](/source/Bibcode_(identifier)):[2022ARNPS..72....1T](https://ui.adsabs.harvard.edu/abs/2022ARNPS..72....1T). [doi](/source/Doi_(identifier)):[10.1146/annurev-nucl-111119-041046](https://doi.org/10.1146%2Fannurev-nucl-111119-041046).

1. ^ [***a***](#cite_ref-Intertwined-2022_113-0) [***b***](#cite_ref-Intertwined-2022_113-1) Abdalla, Elcio; et al. (June 2022). "Cosmology intertwined: A review of the particle physics, astrophysics, and cosmology associated with the cosmological tensions and anomalies". *Journal of High Energy Astrophysics*. **34**: 49–211. [arXiv](/source/ArXiv_(identifier)):[2203.06142](https://arxiv.org/abs/2203.06142). [Bibcode](/source/Bibcode_(identifier)):[2022JHEAp..34...49A](https://ui.adsabs.harvard.edu/abs/2022JHEAp..34...49A). [doi](/source/Doi_(identifier)):[10.1016/j.jheap.2022.04.002](https://doi.org/10.1016%2Fj.jheap.2022.04.002).

1. **[^](#cite_ref-physicsworld_114-0)** Cooper, Keith (6 February 2024). ["Cosmic combat: delving into the battle between dark matter and modified gravity"](https://physicsworld.com/a/cosmic-combat-delving-into-the-battle-between-dark-matter-and-modified-gravity). physicsworld.

## Further reading

- [Halliday, David](/source/David_Halliday_(physicist)); Resnick, Robert; Krane, Kenneth S. (2001). *Physics v. 1*. New York: John Wiley & Sons. [ISBN](/source/ISBN_(identifier)) [978-0-471-32057-9](https://en.wikipedia.org/wiki/Special:BookSources/978-0-471-32057-9).

- Serway, Raymond A.; Jewett, John W. (2004). [*Physics for Scientists and Engineers*](https://archive.org/details/physicssciengv2p00serw) (6th ed.). Brooks/Cole. [ISBN](/source/ISBN_(identifier)) [978-0-534-40842-8](https://en.wikipedia.org/wiki/Special:BookSources/978-0-534-40842-8).

- Tipler, Paul (2004). *Physics for Scientists and Engineers: Mechanics, Oscillations and Waves, Thermodynamics* (5th ed.). W.H. Freeman. [ISBN](/source/ISBN_(identifier)) [978-0-7167-0809-4](https://en.wikipedia.org/wiki/Special:BookSources/978-0-7167-0809-4).

- [Thorne, Kip S.](/source/Kip_Thorne); [Misner, Charles W.](/source/Charles_W._Misner); [Wheeler, John Archibald](/source/John_Archibald_Wheeler) (1973). *Gravitation*. W.H. Freeman. [ISBN](/source/ISBN_(identifier)) [978-0-7167-0344-0](https://en.wikipedia.org/wiki/Special:BookSources/978-0-7167-0344-0).

## External links

**Gravity**  at Wikipedia's [sister projects](https://en.wikipedia.org/wiki/Wikipedia:Wikimedia_sister_projects)

- [Definitions](https://en.wiktionary.org/wiki/gravity) from Wiktionary
- [Media](https://commons.wikimedia.org/wiki/category:Gravitation) from Commons
- [Quotations](https://en.wikiquote.org/wiki/Gravity) from Wikiquote
- [Texts](https://en.wikisource.org/wiki/1911_Encyclop%C3%A6dia_Britannica/Gravitation) from Wikisource
- [Textbooks](https://en.wikibooks.org/wiki/Physics_Study_Guide/Gravity) from Wikibooks
- [Resources](https://en.wikiversity.org/wiki/Gravitation) from Wikiversity
- [Data](https://www.wikidata.org/wiki/Q11412) from Wikidata

- ["Gravitation"](https://www.encyclopediaofmath.org/index.php?title=Gravitation), *[Encyclopedia of Mathematics](/source/Encyclopedia_of_Mathematics)*, [EMS Press](/source/European_Mathematical_Society), 2001 [1994]

- ["Gravitation, theory of"](https://www.encyclopediaofmath.org/index.php?title=Gravitation,_theory_of), *[Encyclopedia of Mathematics](/source/Encyclopedia_of_Mathematics)*, [EMS Press](/source/European_Mathematical_Society), 2001 [1994]

v t e Fundamental interactions of physics Physical forces Strong interaction fundamental residual Electroweak interaction weak interaction electromagnetism Gravitation Hypothetical forces Fifth force Quintessence Glossary of physics Particle physics Philosophy of physics Universe

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[Portals](https://en.wikipedia.org/wiki/Wikipedia:Contents/Portals):
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Authority control databases International GND National United States France BnF data Japan Czech Republic Spain Korea Israel Other IdRef Encyclopedia of Modern Ukraine Yale LUX

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Adapted from the Wikipedia article [Gravity](https://en.wikipedia.org/wiki/Gravity) by Wikipedia contributors ([contributor history](https://en.wikipedia.org/wiki/Gravity?action=history)). Available under [Creative Commons Attribution-ShareAlike 4.0 International](https://creativecommons.org/licenses/by-sa/4.0/). Changes may have been made.