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In physics, action at a distance is the concept that an object can be moved, changed, or otherwise affected without being physically touched (as in mechanical contact) by another object. That is, it is the nonlocal interaction of objects that are separated in space.

This term was used most often in the context of early theories of gravity and electromagnetism to describe how an object responds to the influence of distant objects. For example, Coulomb's law and Newton's law of universal gravitation are such early theories.

More generally "action at a distance" describes the failure of early atomistic and mechanistic theories which sought to reduce all physical interaction to collision. The exploration and resolution of this problematic phenomenon led to significant developments in physics, from the concept of a field, to descriptions of quantum entanglement and the mediator particles of the Standard Model.[1]

Electricity and magnetismEdit

Philosopher William of Ockham discussed action at a distance to explain magnetism and the ability of the Sun to heat the Earth's atmosphere without affecting the intervening space.[2]

Efforts to account for action at a distance in the theory of electromagnetism led to the development of the concept of a field which mediated interactions between currents and charges across empty space. According to field theory we account for the Coulomb (electrostatic) interaction between charged particles through the fact that charges produce around themselves an electric field, which can be felt by other charges as a force. Maxwell directly addressed the subject of action-at-a-distance in chapter 23 of his A Treatise on Electricity and Magnetism in 1873.[3] He began by reviewing the explanation of Ampère's formula given by Gauss and Weber. On page 437 he indicates the physicists' disgust with action at a distance. In 1845 Gauss wrote to Weber desiring "action, not instantaneous, but propagated in time in a similar manner to that of light". This aspiration was developed by Maxwell with the theory of an electromagnetic field described by Maxwell's equations, which used the field to elegantly account for all electromagnetic interactions, as well as light (which, until then, had been seen as a completely unrelated phenomenon). In Maxwell's theory, the field is its own physical entity, carrying momenta and energy across space, and action-at-a-distance is only the apparent effect of local interactions of charges with their surrounding field.

Electrodynamics was later described without fields (in Minkowski space) as the direct interaction of particles with lightlike separation vectors.[dubious ] This resulted in the Fokker-Tetrode-Schwarzschild action integral. This kind of electrodynamic theory is often called "direct interaction" to distinguish it from field theories where action at a distance is mediated by a localized field (localized in the sense that its dynamics are determined by the nearby field parameters).[4] This description of electrodynamics, in contrast with Maxwell's theory, explains apparent action at a distance not by postulating a mediating entity (the field) but by appealing to the natural geometry of special relativity.

Direct interaction electrodynamics is explicitly symmetrical in time, and avoids the infinite energy predicted in the field immediately surrounding point particles. Feynman and Wheeler have shown that it can account for radiation and radiative damping (which had been considered strong evidence for the independent existence of the field). However, various proofs, beginning with that of Dirac, have shown that direct interaction theories (under reasonable assumptions) do not admit Lagrangian or Hamiltonian formulations (these are the so-called No Interaction Theorems). Also significant is the measurement and theoretical description of the Lamb shift which strongly suggests that charged particles interact with their own field. Fields, because of these and other difficulties, have been elevated to the fundamental operators in QFT and modern physics has thus largely abandoned direct interaction theory.

GravityEdit

NewtonEdit

Newton's classical theory of gravity offered no prospect of identifying any mediator of gravitational interaction. His theory assumed that gravitation acts instantaneously, regardless of distance. Kepler's observations gave strong evidence that in planetary motion angular momentum is conserved. (The mathematical proof is valid only in the case of a Euclidean geometry.) Gravity is also known as a force of attraction between two objects because of their mass.

From a Newtonian perspective, action at a distance can be regarded as "a phenomenon in which a change in intrinsic properties of one system induces a change in the intrinsic properties of a distant system, independently of the influence of any other systems on the distant system, and without there being a process that carries this influence contiguously in space and time" (Berkovitz 2008).[5]

A related question, raised by Ernst Mach, was how rotating bodies know how much to bulge at the equator. This, it seems, requires an action-at-a-distance from distant matter, informing the rotating object about the state of the universe. Einstein coined the term Mach's principle for this question.

It is inconceivable that inanimate Matter should, without the Mediation of something else, which is not material, operate upon, and affect other matter without mutual Contact…That Gravity should be innate, inherent and essential to Matter, so that one body may act upon another at a distance thro' a Vacuum, without the Mediation of any thing else, by and through which their Action and Force may be conveyed from one to another, is to me so great an Absurdity that I believe no Man who has in philosophical Matters a competent Faculty of thinking can ever fall into it. Gravity must be caused by an Agent acting constantly according to certain laws; but whether this Agent be material or immaterial, I have left to the Consideration of my readers.[5]

— Isaac Newton, Letters to Bentley, 1692/3

Different authors have attempted to clarify the aspects of remote action and God’s involvement on the basis of textual investigations[6], mainly from the Mathematical Principles of Natural Philosophy[7], Newton’s correspondence with Richard Bentley (1692/93)[8], and Queries that Newton introduced at the end of the Opticks book in the first three editions (between 1704 and 1721)[9].

Andrew Janiak, in Newton as philosopher[10], considered that Newton denied that gravity could be essential to matter, dismissed direct action at a distance, and also rejected the idea of a material substance. But Newton agreed, in Janiak’s view, with an immaterial ether, which he considered that Newton identifies himself with God himself: “Newton obviously thinks that God might be the very “immaterial medium” underlying all gravitational interactions among material bodies.”

Steffen Ducheyne, in Newton on Action at a Distance[11], considered that Newton never accepted direct remote action, only material intervention or immaterial substance.

Hylarie Kochiras, in Gravity and Newton’s substance counting problem[12], argued that Newton was inclined to reject direct action, giving priority to the hypothesis of an intangible environment. But, in his speculative moments, Newton oscillated between accepting and rejecting direct remote action. Newton, according to Kochiras, claims that God is a virtual omnipresent, the force/agent must subsist in substance, and God is omnipresent substantially, resulting in a hidden premise, the principle of local action.

Eric Schliesser, in Newton’s substance monism, distant action, and the nature of Newton’s Empiricism[13], argued that Newton does not categorically refuse the idea that matter is active, and therefore accepted the possibility of a direct action at a distance. Newton affirms the virtual omnipresence of God in addition to his substantial omnipresence.

John Henry, in Gravity and De gravitatione: The Development of Newton’s Ideas on Action at a Distance[14], also argued that direct remote action was not inconceivable for Newton, rejecting the idea that gravity can be explained by subtle matter, accepting the idea of an omnipotent God, and rejecting the Epicurean attraction.

For further discussion see Ducheyne, S. "Newton on Action at a Distance". Journal of the History of Philosophy vol. 52.4 (2014): 675–702.

EinsteinEdit

According to Albert Einstein's theory of special relativity, instantaneous action at a distance violates the relativistic upper limit on speed of propagation of information. If one of the interacting objects were to suddenly be displaced from its position, the other object would feel its influence instantaneously, meaning information had been transmitted faster than the speed of light.

One of the conditions that a relativistic theory of gravitation must meet is that gravity is mediated with a speed that does not exceed c, the speed of light in a vacuum. From the previous success of electrodynamics, it was foreseeable that the relativistic theory of gravitation would have to use the concept of a field, or something similar.

This has been achieved by Einstein's theory of general relativity, in which gravitational interaction is mediated by deformation of space-time geometry. Matter warps the geometry of space-time, and these effects are—as with electric and magnetic fields—propagated at the speed of light. Thus, in the presence of matter, space-time becomes non-Euclidean, resolving the apparent conflict between Newton's proof of the conservation of angular momentum and Einstein's theory of special relativity.

Mach's question regarding the bulging of rotating bodies is resolved because local space-time geometry is informing a rotating body about the rest of the universe. In Newton's theory of motion, space acts on objects, but is not acted upon. In Einstein's theory of motion, matter acts upon space-time geometry, deforming it; and space-time geometry acts upon matter, by affecting the behavior of geodesics.

As a consequence, and unlike the classical theory, general relativity predicts that accelerating masses emit gravitational waves, i.e. disturbances in the curvature of spacetime that propagate outward at lightspeed. Their existence (like many other aspects of relativity) has been experimentally confirmed by astronomers—most dramatically in the direct detection of gravitational waves originating from a black hole merger when they passed through LIGO in 2015.[15]

Quantum mechanicsEdit

Since the early twentieth century, quantum mechanics has posed new challenges for the view that physical processes should obey locality. Whether quantum entanglement counts as action-at-a-distance hinges on the nature of the wave function and decoherence, issues over which there is still considerable debate among scientists and philosophers. One important line of debate originated with Einstein, who challenged the idea that quantum mechanics offers a complete description of reality, along with Boris Podolsky and Nathan Rosen. They proposed a thought experiment involving an entangled pair of observables with non-commuting operators (e.g. position and momentum).[16]

This thought experiment, which came to be known as the EPR paradox, hinges on the principle of locality. A common presentation of the paradox is as follows: two particles interact and fly off in opposite directions. Even when the particles are so far apart that any classical interaction would be impossible (see principle of locality), a measurement of one particle nonetheless determines the corresponding result of a measurement of the other.

After the EPR paper, several scientists such as de Broglie studied local hidden variables theories. In the 1960s John Bell derived an inequality that indicated a testable difference between the predictions of quantum mechanics and local hidden variables theories.[17] To date, all experiments testing Bell-type inequalities in situations analogous to the EPR thought experiment have results consistent with the predictions of quantum mechanics, suggesting that local hidden variables theories can be ruled out. Whether or not this is interpreted as evidence for nonlocality depends on one's interpretation of quantum mechanics.[5]

Non-standard interpretations of quantum mechanics vary in their response to the EPR-type experiments. The Bohm interpretation gives an explanation based on nonlocal hidden variables for the correlations seen in entanglement. Many advocates of the many-worlds interpretation argue that it can explain these correlations in a way that does not require a violation of locality,[18] by allowing measurements to have non-unique outcomes.

See alsoEdit

SourcesEdit

  This article incorporates text from a free content work. Licensed under CC-BY-SA Newton’s action at a distance – Different views, Nicolae Sfetcu, To learn how to add open license text to Wikipedia articles, please see this how-to page. For information on reusing text from Wikipedia, please see the terms of use.

ReferencesEdit

  1. ^ Hesse, Mary B. (December 1955). "Action at a Distance in Classical Physics". Isis. 46 (4): 337–353. doi:10.1086/348429. JSTOR 227576.
  2. ^ Tachau, Katherine H. Vision and Certitude in the Age of Ockham: Optics, Epistemology, and the Foundations of Semantics, 1250–1345. Brill Archive. p. 133. ISBN 9004085521.
  3. ^ Clerk Maxwell (1873) A Treatise on Electricity and Magnetism, pages 426–438, link from Internet Archive
  4. ^ Barut, A. O. "Electrodynamics and Classical Theory of Fields and Particles"
  5. ^ a b c Berkovitz, Joseph (2008). "Action at a Distance in Quantum Mechanics". In Edward N. Zalta (ed.). The Stanford Encyclopedia of Philosophy (Winter 2008 ed.).
  6. ^ "Newton's action at a distance – Different views". SetThings. Retrieved May 29, 2019.
  7. ^ Isaac Newton (1999) The Principia: Mathematical Principles of Natural Philosophy, Univ of California Press
  8. ^ Bentley, Richard (1693) A confutation of atheism from the origin and frame of the world. Part II a sermon preached at St. Martin's in the Fields, November the 7th, 1692 : being the seventh of the lecture founded by the Honourable Robert Boyle ... / by Richard Bentley ..., Ann Arbor, MI ; Oxford (UK) :: Text Creation Partnership, 2007-10 (EEBO-TCP Phase 1)
  9. ^ Isaac Newton (1730) Opticks:: Or, A Treatise of the Reflections, Refractions, Inflections and Colours of Light, William Innys at the West-End of St. Paul's
  10. ^ Andrew Janiak (2008) Newton as Philosopher, Cambridge Core, July 2008
  11. ^ Steffen Ducheyne (2011) Newton on Action at a Distance and the Cause of Gravity, Studies in History and Philosophy of Science Part A 42 (1): 154–59
  12. ^ Hylarie Kochiras (2009) Gravity and Newton’s Substance Counting Problem, Studies in History and Philosophy of Science Part A 40 (3): 267–80
  13. ^ Eric Schliesser (2011) Newton’s Substance Monism, Distant Action, and the Nature of Newton’s Empiricism: Discussion of H. Kochiras ‘Gravity and Newton’s Substance Counting Problem, Studies in History and Philosophy of Science Part A 42 (1): 160–66
  14. ^ John Henry (2011) Gravity and De Gravitatione: The Development of Newton’s Ideas on Action at a Distance, Studies in History and Philosophy of Science Part A 42 (1): 11–27
  15. ^ "Scientists make first direct detection of gravitational waves".
  16. ^ Einstein, A.; Podolsky, B.; Rosen, N. (1935). "Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?" (PDF). Physical Review. 47 (10): 777–780. Bibcode:1935PhRv...47..777E. doi:10.1103/PhysRev.47.777.
  17. ^ Bell, J.S. (1966). On the problem of hidden variables in quantum mechanics. Reviews of Modern Physics. 38(3). 447-452.
  18. ^ Rubin (2001). "Locality in the Everett Interpretation of Heisenberg-Picture Quantum Mechanics". Found. Phys. Lett. 14 (4): 301–322. arXiv:quant-ph/0103079. doi:10.1023/A:1012357515678.

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