In physics,gravity (from Latin gravitas'weight'[1]), also known asgravitation or agravitational interaction,[2] is afundamental interaction, which may be described as the effect of a field that is generated by a gravitational source such as mass.
The gravitational attraction between clouds of primordialhydrogen and clumps ofdark matter in the earlyuniverse caused the hydrogen gas tocoalesce, eventually condensing and fusing toform stars. 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.
Scientists are looking for a theory that describes gravity in the framework ofquantum mechanics (quantum gravity),[4] which would unify gravity and the other known fundamental interactions of physics in a single mathematical framework (atheory of everything).[5]
On the surface of a planetary body such ason Earth, this leads to gravitational acceleration of all objects towards the body, modified by the centrifugal effects arising from the rotation of the body.[6] In this context, gravity givesweight tophysical objects and is essential to understanding the mechanisms that are responsible for surface waterwaves, lunartides and substantially contributes to weather patterns. Gravitational weight also has many important biological functions, helping to guide the growth of plants through the process ofgravitropism and influencing thecirculation of fluids inmulticellular organisms.
Characterization
Gravity is the word used to describe aphysical law, afundamental physical interaction that derives primarily frommass, 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 thegravitational constant,G, as[7]for two masses,m, andm′ separated by a distancer.
Gravity is considered to be one of four fundamental interactions. Theelectromagnetic 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 twoelectrons to their electrical repulsion is 1 to4.17×1042.[7] As a result, gravity can generally be neglected at the level ofsubatomic particles.[8] Gravity becomes the most significant interaction between objects at the scale of astronomical bodies, and it determines the motion ofsatellites,planets,stars,galaxies, and evenlight. Gravity is also fundamental in another sense: theinertial mass that appears inNewton's second law is the same as thegravitational mass. Thisequivalence principle is ascientific hypothesis that has been tested experimentally to more than one part in a trillion.[9]
The nature and mechanism of gravity were explored by a wide range of ancient scholars. InAncient Greece,Aristotle believed that each of theclassical elements had anatural 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.[10] He also thought that the speed of a falling object should increase with its weight, a conclusion that was later shown to be false.[11] While Aristotle's view was widely accepted throughout Ancient Greece, there were other thinkers such asPlutarch who correctly predicted that the attraction of gravity was not unique to the Earth.[12]
Although he did not understand gravity as a force, the ancient Greek philosopherArchimedes discovered thecenter of gravity of a triangle.[13] 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.[14] Two centuries later, the Roman engineer and architectVitruvius contended in hisDe architectura that gravity is not dependent on a substance's weight but rather on its "nature".[15] In the 6th century CE, theByzantine Alexandrian scholarJohn 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.[16]
In 628 CE, theIndian mathematician and astronomerBrahmagupta proposed the idea that gravity is an attractive force that draws objects to the Earth and used the termgurutvākarṣaṇ to describe it.[17]: 105 [18][19]
In the ancientMiddle East, gravity was a topic of fierce debate. ThePersian intellectualAl-Biruni believed that the force of gravity was not unique to the Earth, and he correctly assumed that otherheavenly bodies should exert a gravitational attraction as well.[20] In contrast,Al-Khazini held the same position as Aristotle that all matter in theUniverse is attracted to the center of the Earth.[21]
TheLeaning Tower of Pisa, where according to legend Galileo performed an experiment about the speed of falling objects
In the mid-16th century, various European scientists experimentally disproved theAristotelian notion that heavier objectsfall at a faster rate.[22] In particular, theSpanish Dominican priestDomingo de Soto wrote in 1551 that bodies infree fall uniformly accelerate.[22] De Soto may have been influenced by earlier experiments conducted by otherDominican priests in Italy, including those byBenedetto Varchi, Francesco Beato,Luca Ghini, andGiovan Bellaso which contradicted Aristotle's teachings on the fall of bodies.[22]
The mid-16th century Italian physicistGiambattista Benedetti published papers claiming that, due tospecific gravity, objects made of the same material but with different masses would fall at the same speed.[23] With the 1586Delft tower experiment, theFlemish physicistSimon Stevin observed that two cannonballs of differing sizes and weights fell at the same rate when dropped from a tower.[24]
In the late 16th century,Galileo Galilei's careful measurements of balls rolling downinclines allowed him to firmly establish that gravitational acceleration is the same for all objects.[25][26]: 334 Galileo postulated thatair resistance is the reason that objects with a low density and highsurface area fall more slowly in an atmosphere. In his 1638 workTwo New Sciences, Galileo proved that the distance traveled by a falling object is proportional to thesquare of the time elapsed. His method was a form of graphical numerical integration since concepts of algebra and calculus were unknown at the time.[27]: 4 This was later confirmed by Italian scientistsJesuitsGrimaldi andRiccioli between 1640 and 1650. They also calculated the magnitude ofthe Earth's gravity by measuring the oscillations of a pendulum.[28]
Galileo also broke with incorrect ideas of Aristotelian philosophy by regardinginertia 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 ofreference frame and theprinciple of relativity.[29]: 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.[30]: 17
In last quarter of the 16th centuryTycho Brahe created accurate tools forastrometry, providing careful observations of the planets. His assistant and successor,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.[31]In his 1609 bookAstronomia 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.[32][33]: 846
In 1666,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.[33]: 848
In 1657,Robert Hooke published hisMicrographia, in which he hypothesized that the Moon must have its own gravity.[34]: 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.[35] 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....[36][37]
Hooke was an important communicator who helped reformulate the scientific enterprise.[38] He was one of the first professional scientists and worked as the then-newRoyal Society's curator of experiments for 40 years.[39] However his valuable insights remained hypotheses and some of these were incorrect.[40] He was unable develop a mathematical theory of gravity and work out the consequences.[33]: 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.[38] When Newton reported his results in 1686, Hooke claimed theinverse square law portion was his "notion".
English physicist and mathematician, SirIsaac Newton (1642–1727)
Before 1684, scientists includingChristopher Wren,Robert Hooke andEdmund Halley determined thatKepler's third law, relating to planetary orbital periods, would prove theinverse 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.[30]: 13 In 1684,Isaac Newton sent a manuscript toEdmond Halley titledDe motu corporum in gyrum ('On the motion of bodies in an orbit'), which provided a physical justification forKepler's laws of planetary motion.[41] Halley was impressed by the manuscript and urged Newton to expand on it, and a few years later Newton published a groundbreaking book calledPhilosophiæ 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.[42]: 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".[43]: 546 This formulation had two important parts. First wasequating inertial mass and gravitational mass. Newton's 2nd law defines force via for inertial mass, hislaw of gravitational force uses the same mass. Newton did experiments with pendulums to verify this concept as best he could.[30]: 11
The second aspect of Newton's formulation was the inverse square of distance. This aspect was not new: the astronomerIsmaël 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 theEarth's gravity acts as if all its mass were concentrated at its center. That proof took him twenty years.[30]: 13
Newton'sPrincipia was well received by the scientific community, and his law of gravitation quickly spread across the European world.[44] More than a century later, in 1821, his theory of gravitation rose to even greater prominence when it was used to predict the existence ofNeptune. In that year, the French astronomerAlexis Bouvard used this theory to create a table modeling the orbit ofUranus, 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 astronomersJohn Couch Adams andUrbain 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.[45][46]
Newton's formulation was later condensed into the inverse-square law:whereF is the force,m1 andm2 are the masses of the objects interacting,r is the distance between the centers of the masses andG is thegravitational constant6.674×10−11 m3⋅kg−1⋅s−2.[47] WhileG is also calledNewton'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:Using the values known at the time, Newton was able to verify this form of his law. The value ofG was eventuallymeasured byHenry Cavendish in 1797.[48]: 31
Eventually, astronomers noticed an eccentricity in the orbit of the planetMercury which could not be explained by Newton's theory: theperihelion of the orbit was increasing by about 42.98arcseconds 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 developed a theory ofgeneral relativity which was able to accurately model Mercury's orbit.[49]
The principle of relativity, introduced by Galileo and used as a foundational principle by Newton, led to a long and fruitless search for aluminiferous aether afterMaxwell'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'sspecial relativity theory showed the aether was not needed. Special relativity proposed that mechanics be reformulated to use theLorentz transformation already applicable to light rather than theGalilean transformation adopted by Newton. Special relativity, as inspecial case, specifically did not cover gravity.[30]: 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 was anancient science that gradually broke free of Euclidean limitations whenCarl Gauss discovered in the 1800s thatsurfaces in any number of dimensions could be characterized by ametric, a distance measurement along the shortest path between two points that reduces to Euclidean distance at infinitesimal separation. Gauss' studentBernhard Riemann developed this into a complete geometry by 1854. These geometries are locally flat but have globalcurvature.[30]: 4
In 1907, Einstein took his first step by using special relativity to create a new form of theequivalence principle. The equivalence of inertial mass and gravitational mass was a known empirical law. Them in Newton's first law,, has the same value as them in Newton's law of gravity on Earth,. 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 localgravitational field.[50] Every description of gravity in any other coordinate system must transform to give no field in the free-fall case, a powerfulinvariance constraint on all theories of gravity.[30]: 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 astrophysicistArthur Eddington was able to confirm the predicted deflection of light duringthat year's solar eclipse.[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 physicistsRobert Pound andGlen Rebka performedan experiment in which they usedgamma rays to confirm the prediction ofgravitational time dilation. By sending the rays down a 74-foot tower and measuring their frequency at the bottom, the scientists confirmed that light isDoppler shifted 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 aredshift.[55] Thetime delay of light passing close to a massive object was first identified byIrwin I. Shapiro in 1964 in interplanetary spacecraft signals.[56]
In 1971, scientists discovered the first-ever black hole in the galaxyCygnus. The black hole was detected because it was emitting bursts ofx-rays as it consumed a smaller star, and it came to be known asCygnus 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, the idea that a rotating massive object should twist spacetime around it, was confirmed byGravity Probe B results in 2011.[59][60] In 2015, theLIGO observatory detected faintgravitational waves, the existence of which had been predicted by general relativity. Scientists believe that the waves emanated from ablack hole merger that occurred 1.5 billionlight-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.
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, astandard gravity value is defined by theInternational Bureau of Weights and Measures, under theInternational System of Units (SI).
The force of gravity experienced by objects on Earth's surface is thevector sum 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 thecentrifugal 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]
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 theatmosphere where equilibrium is disturbed by thermalweather fronts or mountain ranges.[67]
Planets orbit theSun in anellipse as a consequence of the law of gravity. Similarly theMoon and artificialsatellites 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]
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 abrown dwarf orgas-giant planet is produced. If more mass is available, the additional gravitational energy allows the central region to reach pressures sufficient fornuclear fusion, forming astar. In a star, again the gravitational attraction competes, with thermal and radiation pressure inhydrostatic 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 aswhite dwarf stars with a small core balancing gravitational attraction withelectron degeneracy pressure. Stars with masses similar to the Sun go through ared giant phase before becoming white dwarf stars. Higher mass stars have complex core structures that burn helium and high atomic number elements ultimately producing aniron core. As their fuel runs out, these stars become unstable producing asupernova. The result can be aneutron star where gravitational attraction balancesneutron degeneracy pressure or, for even higher masses, ablack hole where gravity operates alone with such intensity that even light cannot escape.[68]: 121
TheLIGO 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 theHulse–Taylor binary in 1973. This system consists of apulsar 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 theNobel Prize in Physics in 1993.[69]
The first direct evidence for gravitational radiation was measured on 14 September 2015 by theLIGO 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 andblack hole formation also create detectable amounts of gravitational radiation.[73] This research was awarded the Nobel Prize in Physics in 2017.[74]
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 asdark matter halos attract hydrogen gas leading to stars and galaxies.[75]
Einstein's Cross, four images of the same distantquasar 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 atKitt Peak National Observatory in Arizona, which saw two mirror images of the same quasar whose light had been bent around the galaxyYGKOW 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 likeeyeglass lenses, but rather lead to annular shapes calledEinstein rings.[48]: 370
In October 2017, theLIGO andVirgo interferometer detectors received gravitational wave signals 2 seconds beforegamma 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]
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 todark matter.
Galaxy rotation curves: 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 withingalaxy clusters show a similar pattern. The pattern is considered strong evidence fordark matter, which would interact through gravitation but not electromagnetically; variousmodifications to Newtonian dynamics have also been proposed.[79]
Flyby anomaly: Various spacecraft have experienced greater acceleration than expected duringgravity assist maneuvers.[82] ThePioneer 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 models gravity as a forceF between two objects proportional to their mass,m: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 thisaction at a distance does not explain the root cause of the force, but nevertheless the model explains a vast number of physical effects including cannon ball trajectories, tidal motion and planetary orbits.[85]: 4 However, combining the concept ofrelativity with gravity is enormously complex using this Newtonian model.[85]: 48
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 –discuss] Field models are local: the field values on a sphere completely determine the effects of gravity with the sphere.[85]: 45
A third completely different way to derive a model of gravity is based onaction 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 theLagrangian; 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.[86]: 396 TheEinstein field equation for gravitation can be derived from theEinstein–Hilbert action.[86]: 388
Inmodern physics, general relativity is considered the most successful theory of gravitation.[87] Physicists continue to work to findsolutions to theEinstein field equations that form the basis of general relativity and continue to test the theory, finding excellent agreement in all cases.[88][89][90]: p.9
Constraints
Any theory of gravity must conform to the requirements of special relativity and experimental observations. Newton's theory of gravity assumesaction at a distance and therefore cannot be reconciled with special relativity. The simplest generalization of Newton's approach would be ascalar 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. Avector 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.[91]
General characteristics
Unlike Newton's formula with one parameter,G, force in general relativity is terms of 10 numbers formed in to ametric tensor.[30]: 70 In general relativity the effects of gravitation are described in different ways in different frames of reference. In a free-falling or co-movingcoordinate 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 inspacetime (not 3D space) taken by a free-falling object is called ageodesic 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.[30]: 77
The non-linear second-order Einstein field equations are extremely complex and have been solved in only a few special cases.[94] These cases however have been transformational in our understanding of the cosmos. Several solutions are the basis for understandingblack holes and for our modern model of the evolution of the universe since theBig Bang.[42]: 227
The 1919total 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.[95] A wide range of experiments provided support of general relativity.[90]: 1–9 [96][97][98][99] 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.[90]: 79 [100]
Despite its success in predicting the effects of gravity at large scales, general relativity is ultimately incompatible withquantum 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 asquanta. 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.[101] As a result, researchers have begun to search for a theory that could unite both gravity and quantum mechanics under a more general framework.[102]
One path is to describe gravity in the framework ofquantum field theory (QFT), which has been successful to accurately describe the otherfundamental interactions. The electromagnetic force arises from an exchange of virtualphotons, where the QFT description of gravity is that there is an exchange ofvirtualgravitons.[103][104] This description reproduces general relativity in theclassical limit. However, this approach fails at short distances of the order of thePlanck length,[105] where a more complete theory ofquantum gravity (or a new approach to quantum mechanics) is required.
General relativity has withstood manytests over a large range of mass and size scales.[106][107] When applied to interpret astronomical observations, cosmological models based on general relativity introduce two components to the universe,[108]dark matter[109] anddark energy,[110] the nature of which is currently anunsolved problem in physics. The many successful, high precision predictions of thestandard model of cosmology has led astrophysicists to conclude it and thus general relativity will be the basis for future progress.[111][112] However, dark matter is not supported by theStandard Model of particle physics, physical models for dark energy do not match cosmological data, and some cosmological observations are inconsistent.[112] These issues have led to the study of alternative theories of gravity.[113]
See also
Anti-gravity – Physical and science fiction concept
^Cartwright, Jon (17 May 2025). "Defying gravity".New Scientist. pp. 30–33.
^abHofmann-Wellenhof, B.; Moritz, H. (2006).Physical Geodesy (2nd ed.). Springer.ISBN978-3-211-33544-4.§ 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.
^abcFeynman, Richard P.; Leighton, Robert B.; Sands, Matthew L. (2006)."The Theory of Gravitation".The Feynman lectures on physics (Definitive ed.). San Francisco, Calif.: Pearson Addison Wesley.ISBN978-0-8053-9045-2.
^Vitruvius, Marcus Pollio (1914)."7". 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 on 13 October 2016. Retrieved10 April 2019.
^Rozhanskaya, Mariam; Levinova, I. S. (1996). "Statics". In Rushdī, Rāshid (ed.).Encyclopedia of the History of Arabic Science. Vol. 2. Psychology Press. pp. 614–642.ISBN978-0-415-12411-9.
^Galileo (1638),Two New Sciences, First Day Salviati speaks: "If this were what Aristotle meant you would burden him with another error which would amount to a falsehood; because, since there is no such sheer height available on earth, it is clear that Aristotle could not have made the experiment; yet he wishes to give us the impression of his having performed it when he speaks of such an effect as one which we see."
^Sobel, Dava (1993).Galileo's daughter: a historical memoir of science, faith, and love. New York: Walker.ISBN978-0-8027-1343-8.
^J. L. Heilbron,Electricity in the 17th and 18th Centuries: A Study of Early Modern Physics (Berkeley, California: University of California Press, 1979), p. 180.
^Ferraro, Rafael (2007).Einstein's space-time: an introduction to special and general relativity. New York: Springer.ISBN978-0-387-69946-2.OCLC141385334.
^abcDijksterhuis, E. J. (1954). History of Gravity and Attraction before Newton. Cahiers d'Histoire Mondiale. Journal of World History. Cuadernos de Historia Mundial, 1(4), 839.
^Purrington, Robert D. (2009).The first professional scientist: Robert Hooke and the Royal Society of London. Science networks. Historical studies. Basel, Switzerland Boston: Birkhäuser.ISBN978-3-0346-0037-8.
^Newton, Isaac (1999).The Principia, The Mathematical Principles of Natural Philosophy. Translated by Cohen, I.B.; Whitman, A. Los Angeles: University of California Press.
^Weinberg, Steven (1972).Gravitation and cosmology. John Wiley & Sons.ISBN978-0-471-92567-5.. Quote, p. 192: "About a dozen stars in all were studied, and yielded values 1.98 ± 0.11" and 1.61 ± 0.31", in substantial agreement with Einstein's prediction θ☉ = 1.75"."
^Boynton, Richard (2001)."Precise Measurement of Mass"(PDF).Sawe Paper No. 3147. Arlington, Texas: S.A.W.E., Inc. Archived fromthe original(PDF) on 27 February 2007. Retrieved22 December 2023.
^Young, I. R. (1999).Wind generated ocean waves. Elsevier ocean engineering book series (1st ed.). Amsterdam ; New York: Elsevier.ISBN978-0-08-043317-2.
^"The Nobel Prize in Physics 1993".Nobel Foundation. 13 October 1993.Archived from the original on 10 August 2018. Retrieved22 December 2023.for the discovery of a new type of pulsar, a discovery that has opened up new possibilities for the study of gravitation
Tipler, Paul (2004).Physics for Scientists and Engineers: Mechanics, Oscillations and Waves, Thermodynamics (5th ed.). W.H. Freeman.ISBN978-0-7167-0809-4.