Timeline of gravitational physics and relativity

The following is a timeline of gravitational physics and general relativity.

Before 1500Edit

  • 3rd century BC - Aristarchus of Samos proposes heliocentric model, measures the distance to the Moon and its size

1500sEdit

  • 1543 – Nicolaus Copernicus places the Sun at the gravitational center, starting a revolution in science
  • 1583 – Galileo Galilei induces the period relationship of a pendulum from observations (according to later biographer).
  • 1586 – Simon Stevin demonstrates that two objects of different mass accelerate at the same rate when dropped.
  • 1589 – Galileo Galilei describes a hydrostatic balance for measuring specific gravity.
  • 1590 – Galileo Galilei formulates modified Aristotelean theory of motion (later retracted) based on density rather than weight of objects.

1600sEdit

  • 1602 – Galileo Galilei conducts experiments on pendulum motion.
  • 1604 – Galileo Galilei conducts experiments with inclined planes and induces the law of falling objects.
  • 1607 – Galileo Galilei arrives a mathematical formulation of the law of falling objects based on his earlier experiments.
  • 1608 – Galileo Galilei discovers the parabolic arc of projectiles through experiment.
  • 1609 – Johannes Kepler describes the motion of planets around the Sun, now known as Kepler's laws of planetary motion.
  • 1640 – Ismaël Bullialdus suggests an inverse-square gravitational force law.
  • 1665 – Isaac Newton introduces an inverse-square universal law of gravitation uniting terrestrial and celestial theories of motion and uses it to predict the orbit of the Moon and the parabolic arc of projectiles.
  • 1684 – Isaac Newton proves that planets moving under an inverse-square force law will obey Kepler's laws
  • 1686 – Isaac Newton uses a fixed length pendulum with weights of varying composition to test the weak equivalence principle to 1 part in 1000

1700sEdit

  • 1798 – Henry Cavendish measures the force of gravity between two masses, leading to the first accurate value for the gravitational constant

1800sEdit

  • 1846 – Urbain Le Verrier and John Couch Adams, studying Uranus' orbit, independently prove that another, farther planet must exist. Neptune was found at the predicted moment and position.
  • 1855 – Le Verrier observes a 35 arcsecond per century excess precession of Mercury's orbit and attributes it to another planet, inside Mercury's orbit. The planet was never found. See Vulcan.
  • 1876 – William Kingdon Clifford suggests that the motion of matter may be due to changes in the geometry of space
  • 1882 – Simon Newcomb observes a 43 arcsecond per century excess precession of Mercury's orbit
  • 1887 – Albert A. Michelson and Edward W. Morley in their famous experiment do not detect the ether drift
  • 1889 – Loránd Eötvös uses a torsion balance to test the weak equivalence principle to 1 part in one billion
  • 1893 – Ernst Mach states Mach's principle; first constructive attack on the idea of Newtonian absolute space
  • 1898 – Henri Poincaré states that simultaneity is relative
  • 1899 – Hendrik Antoon Lorentz published Lorentz transformations

1900sEdit

  • 1904 – Henri Poincaré presents the principle of relativity for electromagnetism
  • 1905 – Albert Einstein completes his theory of special relativity and states the law of mass-energy conservation: E=mc2
  • 1907 – Albert Einstein introduces the principle of equivalence of gravitation and inertia and uses it to predict the gravitational redshift
  • 1915 – Albert Einstein completes his theory of general relativity. The new theory explains Mercury's strange motions that baffled Urbain Le Verrier.
  • 1915 – Karl Schwarzschild publishes the Schwarzschild metric about a month after Einstein published his general theory of relativity. This was the first solution to the Einstein field equations other than the trivial flat space solution.
  • 1916 – Albert Einstein shows that the field equations of general relativity admit wavelike solutions
  • 1918 – J. Lense and Hans Thirring find the gravitomagnetic precession of gyroscopes in the equations of general relativity
  • 1919 – Arthur Eddington leads a solar eclipse expedition which claims to detect gravitational deflection of light by the Sun
  • 1921 – Theodor Kaluza demonstrates that a five-dimensional version of Einstein's equations unifies gravitation and electromagnetism
  • 1937 – Fritz Zwicky states that galaxies could act as gravitational lenses
  • 1937 – Albert Einstein, Leopold Infeld, and Banesh Hoffmann show that the geodesic equations of general relativity can be deduced from its field equations

1950sEdit

  • 1953 – P. C. Vaidya Newtonian time in general relativity, Nature, 171, p260.
  • 1956 – John Lighton Synge publishes the first relativity text emphasizing spacetime diagrams and geometrical methods,
  • 1957 – Felix A. E. Pirani uses Petrov classification to understand gravitational radiation,
  • 1957 – Richard Feynman introduces sticky bead argument,
  • 1957 – John Wheeler discusses the breakdown of classical general relativity near singularities and the need for quantum gravity
  • 1959 – Pound–Rebka experiment, first precision test of gravitational redshift,
  • 1959 – Lluís Bel introduces Bel–Robinson tensor and the Bel decomposition of the Riemann tensor,
  • 1959 – Arthur Komar introduces the Komar mass,
  • 1959 – Richard ArnowittStanley Deser and Charles W. Misner developed ADM formalism.

1960sEdit

  • 1960 – Martin Kruskal and George Szekeres independently introduce the Kruskal–Szekeres coordinates for the Schwarzschild vacuum,
  • 1960 – Shapiro effect confirmed,
  • 1960 – Thomas Matthews and Allan R. Sandage associate 3C 48 with a point-like optical image, show radio source can be at most 15 light minutes in diameter,
  • 1960 – Carl H. Brans and Robert H. Dicke introduce Brans–Dicke theory, the first viable alternative theory with a clear physical motivation,
  • 1960 – Ivor M. Robinson and Andrzej Trautman discover the Robinson-Trautman null dust solution[1]
  • 1961 – Pascual Jordan and Jürgen Ehlers develop the kinematic decomposition of a timelike congruence,
  • 1960 – Robert Pound and Glen Rebka test the gravitational redshift predicted by the equivalence principle to approximately 1%
  • 1962 – Roger Penrose and Ezra T. Newman introduce the Newman–Penrose formalism,
  • 1962 – Ehlers and Wolfgang Kundt classify the symmetries of Pp-wave spacetimes,
  • 1962: –Joshua Goldberg and Rainer K. Sachs prove the Goldberg–Sachs theorem,
  • 1962 – Ehlers introduces Ehlers transformations, a new solution generating method,
  • 1962 – Cornelius Lanczos introduces the Lanczos potential for the Weyl tensor,
  • 1962 – Richard ArnowittStanley Deser, and Charles W. Misner introduce the ADM reformulation and global hyperbolicity,
  • 1962 – Yvonne Choquet-Bruhat on Cauchy problem and global hyperbolicity,
  • 1962 – Istvan Ozsvath and Englbert Schücking rediscover the circularly polarized monochromomatic gravitational wave,
  • 1962 – Hans Adolph Buchdahl discovers Buchdahl's theorem,
  • 1962 – Hermann Bondi introduces Bondi mass,
  • 1962 – Robert DickePeter Roll, and R. Krotkov use a torsion fiber balance to test the weak equivalence principle to 2 parts in 100 billion,
  • 1962 - Hermann Bondi, M. G. van der Burg, A. W. Metzner, and Rainer K. Sachs introduce the asymptotic symmetry group of asymptotically flat, Lorentzian spacetimes at null (i.e., light-like) infinity.
  • 1963 – Roy Kerr discovers the Kerr vacuum solution of Einstein's field equations,
  • 1963 – Redshifts of 3C 273 and other quasars show they are very distant; hence very luminous,
  • 1963 – Newman, T. Unti and L.A. Tamburino introduce the NUT vacuum solution,
  • 1963 – Roger Penrose introduces Penrose diagrams and Penrose limits,
  • 1963 – First Texas Symposium on Relativistic Astrophysics held in Dallas, 16–18 December,
  • 1964 – R. W. Sharp and Misner introduce the Misner–Sharp mass,
  • 1964 – M. A. Melvin discovers the Melvin electrovacuum solution (aka the Melvin magnetic universe),
  • 1964 – Irwin Shapiro predicts a gravitational time delay of radiation travel as a test of general relativity
  • 1965 – Roger Penrose proves first of the singularity theorems,
  • 1965 – Newman and others discover the Kerr–Newman electrovacuum solution,
  • 1965 – Penrose discovers the structure of the light cones in gravitational plane wave spacetimes,
  • 1965 – Kerr and Alfred Schild introduce Kerr-Schild spacetime,
  • 1965 – Subrahmanyan Chandrasekhar determines a stability criterion,
  • 1965 – Arno Penzias and Robert Wilson discover the cosmic microwave background radiation,
  • 1965 – Joseph Weber puts the first Weber bar gravitational wave detector into operation
  • 1966 – Sachs and Ronald Kantowski discover the Kantowski-Sachs dust solution,
  • 1967 – Jocelyn Bell and Antony Hewish discover pulsars,
  • 1967 – Robert H. Boyer and R. W. Lindquist introduce Boyer–Lindquist coordinates for the Kerr vacuum,
  • 1967 – Bryce DeWitt publishes on canonical quantum gravity,
  • 1967 – Werner Israel proves the no-hair theorem,
  • 1967 – Kenneth Nordtvedt develops PPN formalism,
  • 1967 – Mendel Sachs publishes factorization of Einstein's field equations,
  • 1967 – Hans Stephani discovers the Stephani dust solution,
  • 1968 – F. J. Ernst discovers the Ernst equation,
  • 1968 – B. Kent Harrison discovers the Harrison transformation, a solution-generating method,
  • 1968 – Brandon Carter solves the geodesic equations for Kerr–Newmann electrovacuum,
  • 1968 – Hugo D. Wahlquist discovers the Wahlquist fluid,
  • 1968 – Irwin Shapiro presents the first detection of the Shapiro delay
  • 1968 – Kenneth Nordtvedt studies a possible violation of the weak equivalence principle for self-gravitating bodies and proposes a new test of the weak equivalence principle based on observing the relative motion of the Earth and Moon in the Sun's gravitational field
  • 1969 – William B. Bonnor introduces the Bonnor beam,
  • 1969 – Joseph Weber reports observation of gravitational waves[2] (a claim now generally discounted),
  • 1969 – Penrose proposes the (weak) cosmic censorship hypothesis and the Penrose process,
  • 1969 – Stephen W. Hawking proves area theorem for black holes,
  • 1969 – Misner introduces the mixmaster universe,

1970sEdit

  • 1970 – Frank J. Zerilli derives the Zerilli equation,
  • 1970 – Vladimir A. BelinskiǐIsaak Markovich Khalatnikov, and Evgeny Lifshitz introduce the BKL conjecture,
  • 1970 – Chandrasekhar pushes on to 5/2 post-Newtonian order,
  • 1970 – Hawking and Penrose prove trapped surfaces must arise in black holes,
  • 1970 – the Kinnersley-Walker photon rocket,
  • 1970 – Peter Szekeres introduces colliding plane waves,
  • 1971 – Peter C. Aichelburg and Roman U. Sexl introduce the Aichelburg–Sexl ultraboost,
  • 1971 – Introduction of the Khan–Penrose vacuum, a simple explicit colliding plane wave spacetime,
  • 1971 – Robert H. Gowdy introduces the Gowdy vacuum solutions (cosmological models containing circulating gravitational waves),
  • 1971 – Cygnus X-1, the first solid black hole candidate, discovered by Uhuru satellite,
  • 1971 – William H. Press discovers black hole ringing by numerical simulation,
  • 1971 – Harrison and Estabrook algorithm for solving systems of PDEs,
  • 1971 – James W. York introduces conformal method generating initial data for ADM initial value formulation,
  • 1971 – Robert Geroch introduces Geroch group and a solution generating method,
  • 1972 – Jacob Bekenstein proposes that black holes have a non-decreasing entropy which can be identified with the area,
  • 1972 – Carter, Hawking and James M. Bardeen propose the four laws of black hole mechanics,
  • 1972 – Sachs introduces optical scalars and proves peeling theorem,
  • 1972 – Rainer Weiss proposes concept of interferometric gravitational wave detector,
  • 1972 – J. C. Hafele and R. E. Keating perform Hafele–Keating experiment,
  • 1972 – Richard H. Price studies gravitational collapse with numerical simulations,
  • 1972 – Saul Teukolsky derives the Teukolsky equation,
  • 1972 – Yakov B. Zel'dovich predicts the transmutation of electromagnetic and gravitational radiation,
  • 1973 – P. C. Vaidya and L. K. Patel introduce the Kerr–Vaidya null dust solution,
  • 1973 – Publication by Charles W. MisnerKip S. Thorne and John A. Wheeler of the treatise Gravitation, the first modern textbook on general relativity,
  • 1973 – Publication by Stephen W. Hawking and George Ellis of the monograph The Large Scale Structure of Space-Time,
  • 1973 – Geroch introduces the GHP formalism,
  • 1974 – Russell Hulse and Joseph Hooton Taylor, Jr. discover the Hulse–Taylor binary pulsar,
  • 1974 – James W. York and Niall Ó Murchadha present the analysis of the initial value formulation and examine the stability of its solutions,
  • 1974 – R. O. Hansen introduces Hansen–Geroch multipole moments,
  • 1974: –Tullio Regge introduces the Regge calculus,
  • 1974 – Hawking discovers Hawking radiation,
  • 1975 – Chandrasekhar and Steven Detweiler compute quasinormal modes,
  • 1975 – Szekeres and D. A. Szafron discover the Szekeres–Szafron dust solutions,
  • 1976 – Penrose introduces Penrose limits (every null geodesic in a Lorentzian spacetime behaves like a plane wave),
  • 1976 – Gravity Probe A experiment confirmed slowing the flow of time caused by gravity matching the predicted effects to an accuracy of about 70 parts per million.
  • 1976 – Robert Vessot and Martin Levine use a hydrogen maser clock on a Scout D rocket to test the gravitational redshift predicted by the equivalence principle to approximately 0.007%
  • 1978 – Penrose introduces the notion of a thunderbolt,
  • 1978 – Belinskiǐ and Zakharov show how to solve Einstein's field equations using the inverse scattering transform; the first gravitational solitons,
  • 1979 – Richard Schoen and Shing-Tung Yau prove the positive mass theorem.
  • 1979 – Dennis WalshRobert Carswell, and Ray Weymann discover the gravitationally lensed quasar Q0957+561

After 1980Edit

  • 1982 – Joseph Taylor and Joel Weisberg show that the rate of energy loss from the binary pulsar PSR B1913+16 agrees with that predicted by the general relativistic quadrupole formula to within 5%
  • 2002 – First data collection of the Laser Interferometer Gravitational-Wave Observatory (LIGO).
  • 2005 – The first stable numerical solutions of a binary black hole orbit are calculated independently by three different research groups.
  • 2007 – End of Gravity Probe B experiment.
  • 2015 – Advanced LIGO reports the first direct detections of gravitational waves (GW150914 and GW151226).
  • 2017 – Advanced LIGO and Fermi Gamma-ray Space Telescope constrain the speed of gravity to 1 part in 10^{15} of the speed of light with GW170817.
  • 2019 – The Event Horizon Telescope images the shadow of supermassive black hole M87*


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