General relativity

General relativity is a theory of gravitation and to understand the background to the theory we have to look at how theories of gravitation developed. Aristotle's notion of the motion of bodies impeded understanding of gravitation for a long time. He believed that force could only be applied by contact; force at a distance being impossible, and a constant force was required to maintain a body in uniform motion.

Copernicus's view of the solar system was important as it allowed sensible consideration of gravitation. Kepler's laws of planetary motion and Galileo's understanding of the motion and falling bodies set the scene for Newton's theory of gravity which was presented in the Principia in 1687. Newton's law of gravitation is expressed by
F=GM1M2d2F = G \Large\frac{M_1 M_2}{d^2}
where FF is the force between the bodies of masses M1,M2M_{1}, M_{2} and dd is the distance between them. GG is the universal gravitational constant.

After receiving their definitive analytic form from Euler, Newton's axioms of motion were reworked by Lagrange, Hamilton, and Jacobi into very powerful and general methods, which employed new analytic quantities, such as potential, related to force but remote from everyday experience. Newton's universal gravitation was considered proved correct, thanks to the work of Clairaut and Laplace. Laplace looked at the stability of the solar system in Traité du Mécanique Céleste in 1799. In fact the so-called three-body problem was extensively studied in the 19th Century and was not properly understood until much later. The study of the gravitational potential allowed variations in gravitation caused by irregularities in the shape of the earth to be studied both practically and theoretically. Poisson used the gravitational potential approach to give an equation which, unlike Newton's, could be solved under rather general conditions.

Newton's theory of gravitation was highly successful. There was little reason to question it except for one weakness which was to explain how each of the two bodies knew the other was there. Some profound remarks about gravitation were made by Maxwell in 1864. His major work A dynamical theory of the electromagnetic field (1864) was written
... to explain the electromagnetic action between distant bodies without assuming the existence of forces capable of acting directly at sensible distances.
At the end of the work Maxwell comments on gravitation.
After tracing to the action of the surrounding medium both the magnetic and the electric attractions and repulsions, and finding them to depend on the inverse square of the distance, we are naturally led to inquire whether the attraction of gravitation, which follows the same law of the distance, is not also traceable to the action of a surrounding medium.
However Maxwell notes that there is a paradox caused by the attraction of like bodies. The energy of the medium must be decreased by the presence of the bodies and Maxwell said
As I am unable to understand in what way a medium can possess such properties, I cannot go further in this direction in searching for the cause of gravitation.
In 1900 Lorentz conjectured that gravitation could be attributed to actions which propagate with the velocity of light. Poincaré, in a paper in July 1905 (submitted days before Einstein's special relativity paper), suggested that all forces should transform according the Lorentz transformations. In this case he notes that Newton's law of gravitation is not valid and proposed gravitational waves which propagated with the velocity of light.

In 1907, two years after proposing the special theory of relativity, Einstein was preparing a review of special relativity when he suddenly wondered how Newtonian gravitation would have to be modified to fit in with special relativity. At this point there occurred to Einstein, described by him as the happiest thought of my life , namely that an observer who is falling from the roof of a house experiences no gravitational field. He proposed the Equivalence Principle as a consequence:-
... we shall therefore assume the complete physical equivalence of a gravitational field and the corresponding acceleration of the reference frame. This assumption extends the principle of relativity to the case of uniformly accelerated motion of the reference frame.
After the major step of the equivalence principle in 1907, Einstein published nothing further on gravitation until 1911. Then he realised that the bending of light in a gravitational field, which he knew in 1907 was a consequence of the equivalence principle, could be checked with astronomical observations. He had only thought in 1907 in terms of terrestrial observations where there seemed little chance of experimental verification. Also discussed at this time is the gravitational redshift, light leaving a massive body will be shifted towards the red by the energy loss of escaping the gravitational field.

Einstein published further papers on gravitation in 1912. In these he realised that the Lorentz transformations will not apply in this more general setting. Einstein also realised that the gravitational field equations were bound to be non-linear and the equivalence principle appeared to only hold locally.

This work by Einstein prompted others to produce gravitational theories. Work by Nordström, Abraham and Mie was all a consequence of Einstein's, so far failed, attempts to find a satisfactory theory. However Einstein realised his problems.
If all accelerated systems are equivalent, then Euclidean geometry cannot hold in all of them.
Einstein then remembered that he had studied Gauss's theory of surfaces as a student and suddenly realised that the foundations of geometry have physical significance. He consulted his friend Grossmann who was able to tell Einstein of the important developments of Riemann, Ricci (Ricci-Curbastro) and Levi-Civita. Einstein wrote
... in all my life I have not laboured nearly so hard, and I have become imbued with great respect for mathematics, the subtler part of which I had in my simple-mindedness regarded as pure luxury until now.
In 1913 Einstein and Grossmann published a joint paper where the tensor calculus of Ricci and Levi-Civita is employed to make further advances. Grossmann gave Einstein the Riemann-Christoffel tensor which, together with the Ricci tensor which can be derived from it, were to become the major tools in the future theory. Progress was being made in that gravitation was described for the first time by the metric tensor but still the theory was not right. When Planck visited Einstein in 1913 and Einstein told him the present state of his theories Planck said
As an older friend I must advise you against it for in the first place you will not succeed, and even if you succeed no one will believe you.
Planck was wrong, but only just, for when Einstein was to succeed with his theory it was not readily accepted. It was the second half of 1915 that saw Einstein finally put the theory in place. Before that however he had written a paper in October 1914 nearly half of which is a treatise on tensor analysis and differential geometry. This paper led to a correspondence between Einstein and Levi-Civita in which Levi-Civita pointed out technical errors in Einstein's work on tensors. Einstein was delighted to be able to exchange ideas with Levi-Civita whom he found much more sympathetic to his ideas on relativity than his other colleagues.

At the end of June 1915 Einstein spent a week at Göttingen where he lectured for six 2 hour sessions on his (incorrect) October 1914 version of general relativity. Hilbert and Klein attended his lectures and Einstein commented after leaving Göttingen
To my great joy, I succeeded in convincing Hilbert and Klein completely.
The final steps to the theory of general relativity were taken by Einstein and Hilbert at almost the same time. Both had recognised flaws in Einstein's October 1914 work and a correspondence between the two men took place in November 1915. How much they learnt from each other is hard to measure but the fact that they both discovered the same final form of the gravitational field equations within days of each other must indicate that their exchange of ideas was helpful.

On the 18th November he made a discovery about which he wrote For a few days I was beside myself with joyous excitement . The problem involved the advance of the perihelion of the planet Mercury. Le Verrier, in 1859, had noted that the perihelion (the point where the planet is closest to the sun) advanced by 38" per century more than could be accounted for from other causes. Many possible solutions were proposed, Venus was 10% heavier than was thought, there was another planet inside Mercury's orbit, the sun was more oblate than observed, Mercury had a moon and, really the only one not ruled out by experiment, that Newton's inverse square law was incorrect. This last possibility would replace the 1d2\large\frac{1}{d^{2}\normalsize} by 1dp\large\frac{1}{d^{p}\normalsize}, where p=2+ϵp = 2+\epsilon for some very small number ϵ\epsilon. By 1882 the advance was more accurately known, 43'' per century. From 1911 Einstein had realised the importance of astronomical observations to his theories and he had worked with Freundlich to make measurements of Mercury's orbit required to confirm the general theory of relativity. Freundlich confirmed 43" per century in a paper of 1913. Einstein applied his theory of gravitation and discovered that the advance of 43" per century was exactly accounted for without any need to postulate invisible moons or any other special hypothesis. Of course Einstein's 18 November paper still does not have the correct field equations but this did not affect the particular calculation regarding Mercury. Freundlich attempted other tests of general relativity based on gravitational redshift, but they were inconclusive.

Also in the 18 November paper Einstein discovered that the bending of light was out by a factor of 2 in his 1911 work, giving 1.74". In fact after many failed attempts (due to cloud, war, incompetence etc.) to measure the deflection, two British expeditions in 1919 were to confirm Einstein's prediction by obtaining 1.98" ± 0.30" and 1.61" ± 0.30".

On 25 November Einstein submitted his paper The field equations of gravitation which give the correct field equations for general relativity. The calculation of bending of light and the advance of Mercury's perihelion remained as he had calculated it one week earlier.

Five days before Einstein submitted his 25 November paper Hilbert had submitted a paper The foundations of physics which also contained the correct field equations for gravitation. Hilbert's paper contains some important contributions to relativity not found in Einstein's work. Hilbert applied the variational principle to gravitation and attributed one of the main theorem's concerning identities that arise to Emmy Noether who was in Göttingen in 1915. No proof of the theorem is given. Hilbert's paper contains the hope that his work will lead to the unification of gravitation and electromagnetism.

In fact Emmy Noether's theorem was published with a proof in 1918 in a paper which she wrote under her own name. This theorem has become a vital tool in theoretical physics. A special case of Emmy Noether's theorem was written down by Weyl in 1917 when he derived from it identities which, it was later realised, had been independently discovered by Ricci in 1889 and by Bianchi (a pupil of Klein) in 1902.

Immediately after Einstein's 1915 paper giving the correct field equations, Karl Schwarzschild found in 1916 a mathematical solution to the equations which corresponds to the gravitational field of a massive compact object. At the time this was purely theoretical work but, of course, work on neutron stars, pulsars and black holes relied entirely on Schwarzschild's solutions and has made this part of the most important work going on in astronomy today.

Einstein had reached the final version of general relativity after a slow road with progress but many errors along the way. In December 1915 he said of himself
That fellow Einstein suits his convenience. Every year he retracts what he wrote the year before.
Most of Einstein's colleagues were at a loss to understand the quick succession of papers, each correcting, modifying and extending what had been done earlier. In December 1915 Ehrenfest wrote to Lorentz referring to the theory of November 25, 1915. Ehrenfest and Lorentz corresponded about the general theory of relativity for two months as they tried to understand it. Eventually Lorentz understood the theory and wrote to Ehrenfest saying I have congratulated Einstein on his brilliant results . Ehrenfest responded
Your remark "I have congratulated Einstein on his brilliant results" has a similar meaning for me as when one Freemason recognises another by a secret sign.
In March 1916 Einstein completed an article explaining general relativity in terms more easily understood. The article was well received and he then wrote another article on relativity which was widely read and went through over 20 printings.

Today relativity plays a role in many areas, cosmology, the big bang theory etc. and now has been checked by experiment to a high degree of accuracy.

References (show)

  1. A Ashtekar, Chandrasekhar's contributions to general relativity, Current Sci. 70 (9) (1996), 800-804.
  2. C Cattani, Early debates on general relativity in Italy, in General relativity and gravitational physics (River Edge, NJ, 1994), 93-110.
  3. S Chandrasekhar, Einstein and general relativity : historical perspectives, Amer. J. Phys. 47 (3) (1979), 212-217.
  4. J Earman, M Janssen and J D Norton (eds.), The Attraction of gravitation : new studies in the history of general relativity (Boston, 1993).
  5. J Eisenstaedt, La relativité générale à l'étiage : 1925-1955, Archive for History of Exact Sciences 35 (2) (1986), 115-185.
  6. J Eisenstaedt, The low water mark of general relativity, 1925-1955, in Einstein and the history of general relativity (Boston, MA, 1989), 277-292.
  7. J Eisenstaedt and A J Kox (eds.), Studies in the history of general relativity (Boston, 1992).
  8. J Earman and C Glymour, The gravitational red shift as a test of general relativity : history and analysis, Stud. Hist. Philos. Sci. 11 (3) (1980), 175-214.
  9. J Earman and C Glymour, Einstein and Hilbert : two months in the history of general relativity, Archive for History of Exact Sciences 19 (3) (1978/79), 291-308.
  10. R Farwell and C Knee, The end of the absolute : a nineteenth-century contribution to general relativity, Stud. Hist. Philos. Sci. 21 (1) (1990), 91-121.
  11. F R Hickman, Electrodynamical origins of Einstein's theory of general relativity, Internat. J. Theoret. Phys. 23 (6) (1984), 535-566.
  12. D Howard, Einstein and Eindeutigkeit : a neglected theme in the philosophical background to general relativity, in Studies in the history of general relativity (Boston, MA, 1992), 154-243.
  13. D Howard and J Stachel (eds.), Einstein and the history of general relativity (Boston, 1989).
  14. J Illy, Einstein teaches Lorentz, Lorentz teaches Einstein : Their collaboration in general relativity, 1913-1920, Archive for History of Exact Sciences 39 (3) (1989), 247-289.
  15. P Kerszberg, The relativity of rotation in the early foundations of general relativity, Stud. Hist. Philos. Sci. 18 (1) (1987), 53-79.
  16. C W Kilmister, Relativity, in I Grattan-Guinness (ed.), Companion Encyclopedia of the History and Philosophy of the Mathematical Sciences (London, 1994), 1235-1241.
  17. A J Kox, Einstein, Lorentz, Leiden and general relativity, Les Journées Relativistes, Classical Quantum Gravity 10 (1993), S187-S191.
  18. A J Kox, General relativity in the Netherlands, 1915-1920 in Studies in the history of general relativity (Boston, MA, 1992), 39-56.
  19. A Lichnerowicz, Mathematics and general relativity : a recollection, in Studies in the history of general relativity (Boston, MA, 1992), 103-108.
  20. M De Maria, The first reactions to general relativity in Italy : the polemics between Max Abraham and Albert Einstein (Italian), Italian mathematics between the two world wars (Bologna, 1987), 143-159.
  21. J Mehra, Origins of the modern theory of gravitation : the historical origins of the theory of general relativity from 1907 to 1919, Bull. Soc. Roy. Sci. Liège 43 (1974), 190-213.
  22. A Mercier, General relativity at the turning point of its renewal, in Studies in the history of general relativity (Boston, MA, 1992), 109-121.
  23. F Morgan, Calculus, planets, and general relativity, SIAM Rev. 34 (2) (1992), 295-299.
  24. J Norton, Einstein's discovery of the field equations of general relativity : some milestones, Proceedings of the fourth Marcel Grossmann meeting on general relativity (Amsterdam-New York, 1986), 1837-1848.
  25. A Pais, 'Subtle is the Lord...' The Science and the life of Albert Einstein (Oxford, 1982).
  26. J M Sánchez-Ron, The reception of general relativity among British physicists and mathematicians (1915-1930), in Studies in the history of general relativity (Boston, MA, 1992), 57-88.
  27. J J Stachel, How Einstein discovered general relativity : a historical tale with some contemporary morals, General relativity and gravitation (Cambridge-New York, 1987), 200-208.
  28. C Vilain, Spherical coordinates in general relativity from 1915 to 1960 : a physical interpretation, in Studies in the history of general relativity (Boston, MA, 1992), 419-434.
  29. C M Will, General relativity at 75 : how right was Einstein?, in The Sixth Marcel Grossmann Meeting (River Edge, NJ, 1992), 769-786.

Written by J J O'Connor and E F Robertson
Last Update May 1996