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Absolute space and time
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Absolute space and time is a concept in physics and philosophy about the properties of the universe. In physics, absolute space and time may be a preferred frame.
Early concept
[edit]A version of the concept of absolute space (in the sense of a preferred frame) can be seen in Aristotelian physics.[1] Robert S. Westman writes that a "whiff" of absolute space can be observed in Copernicus's De revolutionibus orbium coelestium, where Copernicus uses the concept of an immobile sphere of stars.[2]
Newton
[edit]Originally introduced by Sir Isaac Newton in Philosophiæ Naturalis Principia Mathematica, the concepts of absolute time and space provided a theoretical foundation that facilitated Newtonian mechanics.[3] According to Newton, absolute time and space respectively are independent aspects of objective reality:[4]
Absolute, true and mathematical time, of itself, and from its own nature flows equably without regard to anything external, and by another name is called duration: relative, apparent and common time, is some sensible and external (whether accurate or unequable) measure of duration by the means of motion, which is commonly used instead of true time ...
According to Newton, absolute time exists independently of any perceiver and progresses at a consistent pace throughout the universe. Unlike relative time, Newton believed absolute time was imperceptible and could only be understood mathematically. According to Newton, humans are only capable of perceiving relative time, which is a measurement of perceivable objects in motion (like the Moon or Sun). From these movements, we infer the passage of time.
Absolute space, in its own nature, without regard to anything external, remains always similar and immovable. Relative space is some movable dimension or measure of the absolute spaces; which our senses determine by its position to bodies: and which is vulgarly taken for immovable space ... Absolute motion is the translation of a body from one absolute place into another: and relative motion, the translation from one relative place into another ...
— Isaac Newton
These notions imply that absolute space and time do not depend upon physical events, but are a backdrop or stage setting within which physical phenomena occur. Thus, every object has an absolute state of motion relative to absolute space, so that an object must be either in a state of absolute rest, or moving at some absolute speed.[5] To support his views, Newton provided some empirical examples: according to Newton, a solitary rotating sphere can be inferred to rotate about its axis relative to absolute space by observing the bulging of its equator, and a solitary pair of spheres tied by a rope can be inferred to be in absolute rotation about their center of gravity (barycenter) by observing the tension in the rope.
Differing views
[edit]
Historically, there have been differing views on the concept of absolute space and time. Gottfried Leibniz was of the opinion that space made no sense except as the relative location of bodies, and time made no sense except as the relative movement of bodies.[6] George Berkeley suggested that, lacking any point of reference, a sphere in an otherwise empty universe could not be conceived to rotate, and a pair of spheres could be conceived to rotate relative to one another, but not to rotate about their center of gravity,[7] an example later raised by Albert Einstein in his development of general relativity.
A more recent form of these objections was made by Ernst Mach. Mach's principle proposes that mechanics is entirely about relative motion of bodies and, in particular, mass is an expression of such relative motion. So, for example, a single particle in a universe with no other bodies would have zero mass. According to Mach, Newton's examples simply illustrate relative rotation of spheres and the bulk of the universe.[8]
When, accordingly, we say that a body preserves unchanged its direction and velocity in space, our assertion is nothing more or less than an abbreviated reference to the entire universe.
—Ernst Mach[9]
These views opposing absolute space and time may be seen from a modern stance as an attempt to introduce operational definitions for space and time, a perspective made explicit in the special theory of relativity.
Even within the context of Newtonian mechanics, the modern view is that absolute space is unnecessary. Instead, the notion of inertial frame of reference has taken precedence, that is, a preferred set of frames of reference that move uniformly with respect to one another. The laws of physics transform from one inertial frame to another according to Galilean relativity, leading to the following objections to absolute space, as outlined by Milutin Blagojević:[10]
- The existence of absolute space contradicts the internal logic of classical mechanics since, according to Galilean principle of relativity, none of the inertial frames can be singled out.
- Absolute space does not explain inertial forces since they are related to acceleration with respect to any one of the inertial frames.
- Absolute space acts on physical objects by inducing their resistance to acceleration but it cannot be acted upon.
Newton himself recognized the role of inertial frames.[11]
The motions of bodies included in a given space are the same among themselves, whether that space is at rest or moves uniformly forward in a straight line.
As a practical matter, inertial frames often are taken as frames moving uniformly with respect to the fixed stars.[12] See Inertial frame of reference for more discussion on this.
Mathematical definitions
[edit]Space, as understood in Newtonian mechanics, is three-dimensional and Euclidean, with a fixed orientation. It is denoted E3. If some point O in E3 is fixed and defined as an origin, the position of any point P in E3 is uniquely determined by its radius vector (the origin of this vector coincides with the point O and its end coincides with the point P). The three-dimensional linear vector space R3 is a set of all radius vectors. The space R3 is endowed with a scalar product ⟨ , ⟩.
Time is a scalar which is the same in all space E3 and is denoted as t. The ordered set { t } is called a time axis.
Motion (also path or trajectory) is a function r : Δ → R3 that maps a point in the interval Δ from the time axis to a position (radius vector) in R3.
The above four concepts are the "well-known" objects mentioned by Isaac Newton in his Principia:
- I do not define time, space, place and motion, as being well known to all.[13]
Special relativity
[edit]The concepts of space and time were separate in physical theory prior to the advent of special relativity theory, which connected the two and showed both to be dependent upon the reference frame's motion. In Einstein's theories, the ideas of absolute time and space were superseded by the notion of spacetime in special relativity, and curved spacetime in general relativity.
Absolute simultaneity refers to the concurrence of events in time at different locations in space in a manner agreed upon in all frames of reference. The theory of relativity does not have a concept of absolute time because there is a relativity of simultaneity. An event that is simultaneous with another event in one frame of reference may be in the past or future of that event in a different frame of reference,[6]: 59 which negates absolute simultaneity.
Einstein
[edit]Quoted below from his later papers, Einstein identified the term aether with "properties of space", a terminology that is not widely used. Einstein stated that in general relativity the "aether" is not absolute anymore, as the geodesic and therefore the structure of spacetime depends on the presence of matter.[14]
To deny the ether is ultimately to assume that empty space has no physical qualities whatever. The fundamental facts of mechanics do not harmonize with this view. For the mechanical behaviour of a corporeal system hovering freely in empty space depends not only on relative positions (distances) and relative velocities, but also on its state of rotation, which physically may be taken as a characteristic not appertaining to the system in itself. In order to be able to look upon the rotation of the system, at least formally, as something real, Newton objectivises space. Since he classes his absolute space together with real things, for him rotation relative to an absolute space is also something real. Newton might no less well have called his absolute space “Ether”; what is essential is merely that besides observable objects, another thing, which is not perceptible, must be looked upon as real, to enable acceleration or rotation to be looked upon as something real.
— Albert Einstein, Ether and the Theory of Relativity (1920)[15]
Because it was no longer possible to speak, in any absolute sense, of simultaneous states at different locations in the aether, the aether became, as it were, four-dimensional, since there was no objective way of ordering its states by time alone. According to special relativity too, the aether was absolute, since its influence on inertia and the propagation of light was thought of as being itself independent of physical influence....The theory of relativity resolved this problem by establishing the behaviour of the electrically neutral point-mass by the law of the geodetic line, according to which inertial and gravitational effects are no longer considered as separate. In doing so, it attached characteristics to the aether which vary from point to point, determining the metric and the dynamic behaviour of material points, and determined, in their turn, by physical factors, namely the distribution of mass/energy. Thus the aether of general relativity differs from those of classical mechanics and special relativity in that it is not ‘absolute’ but determined, in its locally variable characteristics, by ponderable matter.
— Albert Einstein, Über den Äther (1924)[16]
General relativity
[edit]Special relativity eliminates absolute time (although Gödel and others suspect absolute time may be valid for some forms of general relativity)[17] and general relativity further reduces the physical scope of absolute space and time through the concept of geodesics.[6]: 207–223 There appears to be absolute space in relation to the distant stars because the local geodesics eventually channel information from these stars, but it is not necessary to invoke absolute space with respect to any system's physics, as its local geodesics are sufficient to describe its spacetime.[18]
See also
[edit]References and notes
[edit]- ^ "Absolute and Relational Space and Motion: Classical Theories". Stanford Encyclopedia of Philosophy. 19 July 2021.
- ^ Robert S. Westman, The Copernican Achievement, University of California Press, 1975, p. 45.
- ^ Knudsen, Jens M.; Hjorth, Poul (2012). Elements of Newtonian Mechanics (illustrated ed.). Springer Science & Business Media. p. 30. ISBN 978-3-642-97599-8.
- ^ Newton, Isaac; Chittenden, N. W. Life of Sir Isaac Newton; Adee, Daniel; Motte, Andrew; Hill, Theodore Preston Early American mathematics books CU-BANC (1846). Newton's Principia : the mathematical principles of natural philosophy. University of California Libraries. New-York : Published by Daniel Adee.
- ^ Space and Time: Inertial Frames (Stanford Encyclopedia of Philosophy)
- ^ a b c Ferraro, Rafael (2007), Einstein's Space-Time: An Introduction to Special and General Relativity, Springer Science & Business Media, Bibcode:2007esti.book.....F, ISBN 9780387699462
- ^ Davies, Paul; Gribbin, John (2007). The Matter Myth: Dramatic Discoveries that Challenge Our Understanding of Physical Reality. Simon & Schuster. p. 70. ISBN 978-0-7432-9091-3.
- ^ Ernst Mach; as quoted by Ignazio Ciufolini; John Archibald Wheeler (1995). Gravitation and Inertia. Princeton University Press. pp. 386–387. ISBN 978-0-691-03323-5.
- ^ as quoted by Ciufolini and Wheeler: Gravitation and Inertia, p. 387
- ^ Blagojević, Milutin (2002). Gravitation and Gauge Symmetries. CRC Press. p. 5. ISBN 978-0-7503-0767-3.
- ^ Newton, Isaac; Chittenden, N. W. Life of Sir Isaac Newton; Adee, Daniel; Motte, Andrew; Hill, Theodore Preston Early American mathematics books CU-BANC (1846). Newton's Principia : the mathematical principles of natural philosophy. University of California Libraries. New-York : Published by Daniel Adee. p. 88.
- ^ Møller, C. (1976). The Theory of Relativity (Second ed.). Oxford, UK: Oxford University Press. p. 1. ISBN 978-0-19-560539-6. OCLC 220221617.
- ^ Newton 1687 Philosophiae Naturalis Principia Mathematica, Londini, Jussu Societatis Regiae ac Typis J. Streater, or The Mathematical Principles of Natural Philosophy, London, English translation by Andrew Motte 1700s. From part of the Scholium, reprinted on page 737 of On the Shoulders of Giants:The Great Works of Physics and Astronomy (works by Copernicus, Kepler, Galileo, Newton, and Einstein). Stephen Hawking, ed. 2002 ISBN 0-7624-1348-4
- ^ Kostro, L. (2001), "Albert Einstein's New Ether and his General Relativity" (PDF), Proceedings of the Conference of Applied Differential Geometry: 78–86, archived from the original (PDF) on 2010-08-02.
- ^ Einstein, Albert: "Ether and the Theory of Relativity" (1920), Sidelights on Relativity (Methuen, London, 1922)
- ^ A. Einstein (1924), "Über den Äther", Verhandlungen der Schweizerischen Naturforschenden Gesellschaft, 105 (2): 85–93. English translation: Concerning the Aether Archived 2010-11-04 at the Wayback Machine
- ^ Savitt, Steven F. (September 2000), "There's No Time Like the Present (in Minkowski Spacetime)", Philosophy of Science, 67 (S1): S563 – S574, CiteSeerX 10.1.1.14.6140, doi:10.1086/392846, S2CID 121275903
- ^ Gilson, James G. (September 1, 2004), Mach's Principle II, arXiv:physics/0409010, Bibcode:2004physics...9010G
External links
[edit]
Media related to Absolute space and time at Wikimedia Commons
Absolute space and time
View on GrokipediaHistorical Development
Early Concepts
The concept of space and time in ancient Greek philosophy laid foundational intuitions for later absolute notions, emphasizing unchanging frameworks underlying motion and change. Plato, in his dialogue Timaeus, introduced space as the chōra or receptacle—a formless, eternal matrix that receives and nurtures the ideal Forms, providing an invariant backdrop for the sensible world's becoming.[3] This receptacle implies a stable spatial structure independent of the transient objects it contains, while time is depicted as a "moving image of eternity," created alongside the cosmos to mimic the timeless perfection of the Forms.[3] Aristotle, building on but critiquing Platonic idealism, defined place (topos) in Physics Book IV as the innermost boundary of the containing body, serving as the arena for natural locomotion and motion.[4] For Aristotle, space thus functions as a relational system of places ordered by the cosmos's spherical structure, with time as the measure of change in this plenum, where void has no existence.[5] In medieval scholasticism, these Greek ideas were synthesized with Christian theology, positing an absolute divine dimension to space and time. Thomas Aquinas, in his Commentary on Aristotle's Physics, integrated Aristotelian physics by viewing place and time as real but created entities, subordinate to God's eternal immensity.[6] Space, for Aquinas, reflects divine omnipresence as an infinite, immaterial expanse encompassing the finite Aristotelian universe, while time derives from mutable creation yet measures motion within God's unchanging eternity.[6] This theological overlay elevated space to an absolute, God-sustained container, bridging Aristotelian relational places with a transcendent framework that ensures cosmic order under divine providence. Pre-scientific intuitions further reinforced absolute space as a fixed, empty backdrop against which objects and events occur, and time as a uniform, irreversible flow independent of observers. These everyday notions, evident in commonsense perceptions of a stable environment for daily motions and a steady progression of moments, predated rigorous analysis and permeated philosophical thought. During the Renaissance transition, Galileo Galilei shifted emphasis to kinematics in works like Two New Sciences, treating space as an isotropic Euclidean arena for describing uniform motion without explicitly invoking absoluteness, yet implicitly assuming a neutral frame for relative velocities.[7] In the mid-17th century, René Descartes further developed these ideas in his Principia Philosophiae (1644), identifying space with the extension of matter and rejecting the existence of void; he treated space relationally as determined by the positions and relations among extended bodies, influencing the debates that Newton would later address.[8]Newton's Formulation
Isaac Newton first elaborated his views on absolute space, time, and motion in the unpublished manuscript De gravitatione et aequipondio fluidorum (commonly referred to as De Gravitatione), composed in the mid-1680s (circa 1684–1685). This work, primarily a philosophical critique of Descartes' identification of motion with change of place relative to immediately contiguous bodies, defined absolute space as an absolutely immovable entity distinct from matter, absolute time as flowing uniformly and equably without relation to anything external, and absolute motion as the translation of a body from one absolute place to another within immovable space. These conceptions implied absolute velocities as rates of change of position relative to absolute space, providing motion with determinate speed and direction in contrast to purely relative accounts, which Newton argued fail to define velocity or trajectory coherently.[2][9] These ideas received their mature and concise expression in the Scholium following the Definitions in his Philosophiæ Naturalis Principia Mathematica, published in 1687 during the Scientific Revolution. There, he defined absolute space as "of its own nature, without relation to anything external, always remains similar and immovable," distinguishing it from relative space, which is "some movable dimension or measure of the absolute space" perceptible through positions relative to bodies. Similarly, absolute time was described as "of itself, and from its own nature, [flowing] equably without relation to anything external," in contrast to relative time, which serves as a "sensible and external measure of duration by means of motion." These definitions provided a foundational framework for Newton's mechanics, independent of observable changes or moving objects.[1] Newton integrated absolute space into his first law of motion, stating that a body persists in its state of rest or uniform rectilinear motion unless compelled to change by impressed forces, with such motion understood relative to absolute space. This absolute reference frame was essential for distinguishing true motion from apparent motion, as relative motions alone could not account for inertial effects. To illustrate, Newton invoked the rotating bucket experiment: a bucket filled with water, suspended by a twisted cord and released to spin, initially keeps the water surface flat while the bucket rotates, but as the water acquires the rotation, its surface becomes concave due to centrifugal forces arising from rotation relative to absolute space, not merely relative to the bucket or surroundings. This demonstrates that true rotational motion produces observable effects independent of external relations, affirming the existence of an immovable absolute space.[1] Underlying these scientific formulations were Newton's theological views, where absolute space served as the divine medium for God's omnipresence. In the General Scholium of the Principia, he asserted that God "endures from eternity to eternity, and is present from infinity to infinity," constituting duration and space as emanations of His being. Newton further elaborated this in the Opticks (1704), describing infinite space as God's "sensorium," an immaterial perceptive organ through which the divine intimately senses all things without reliance on material intermediaries. This perspective reconciled the immutability of absolute space and time with a theistic cosmology, positioning them as eternal attributes enabling God's eternal governance over the universe.Philosophical Debates
Relational Alternatives
Relational theories of space and time, in contrast to absolute conceptions, posit that space and time emerge solely from the relations among material objects and events, lacking any independent existence. Gottfried Wilhelm Leibniz articulated this relationalist view in the early 18th century, defining space as the order of coexistences among phenomena and time as the order of non-coexistences or successive phenomena.[10] According to Leibniz, these relational orders are ideal abstractions derived from the positions and sequences of bodies, rather than entities subsisting on their own.[11] This perspective came into sharp focus during the 1715–1716 correspondence between Leibniz and Samuel Clarke, who defended Isaac Newton's absolute views. Clarke argued that absolute space was essential to God's immensity, equating infinite space with divine omnipresence and warning that Leibniz's relationalism would reduce God to a limited, material-dependent being.[12] Leibniz countered that space and time as relations preserved God's transcendence, avoiding the notion of an empty, infinite container that might imply divine limitation or multiplicity.[13] In the late 19th century, Ernst Mach revived and extended relational critiques in his 1883 work The Science of Mechanics, challenging the Newtonian idea of inertia as defined relative to absolute space. Mach proposed instead that inertial effects arise from the relative motions of bodies with respect to the entire fixed distribution of distant stars and matter in the universe.[14] This "Machian" relationalism emphasized that all motion, including inertial frames, must be empirically grounded in observable cosmic relations, influencing later thinkers like Albert Einstein.[15] Philosophically, relationalism resolves paradoxes associated with absolute space, such as the unintelligibility of empty space existing without objects to relate, by deriving spatial and temporal structures entirely from material interactions.[16] It also aligns with empiricist principles, as space and time become verifiable through the observable relations between events and bodies, eschewing unobservable absolute entities.[11]Key Criticisms
One of the primary logical challenges to Newton's concept of absolute space arose from its inherent unobservability, rendering it undetectable through sensory experience or empirical means. George Berkeley, in his 1721 treatise De Motu, argued that absolute space and motion are metaphysical fictions, as they cannot be perceived or distinguished from relative positions and motions; instead, all motion is relative to other bodies, aligning with an idealist critique that dismissed absolute space as an unnecessary and unverifiable entity beyond human perception.[17] This detectability problem highlighted a fundamental flaw: if absolute space exists, it should in principle allow for the identification of true motion independent of relative observations, yet no such distinction proves possible in practice. Empirical critiques further undermined absolute space by demonstrating that rotational motion, posited by Newton as evidence of absolute rotation, lacked clear observable markers distinguishing it from relative effects. Christiaan Huygens, in his analysis of pendulum behavior in rotating systems during the late 17th century, questioned whether absolute rotation could be confirmed without reference to surrounding matter, noting that phenomena like centrifugal deviation in a rotating pendulum could be interpreted as relative interactions rather than proof of an absolute frame; this suggested that no experiment could unequivocally isolate absolute rotation from observable relative differences.[18] Huygens's work thus challenged Newton's bucket experiment by proposing that rotational dynamics are better understood through relative inertial structures defined by the distribution of matter, rather than an unobservable absolute space.[19] Metaphysical objections portrayed absolute space as an occult, superfluous substance that contravened principles of parsimony, such as Occam's razor, by introducing an invisible, infinite entity without explanatory necessity. In the 18th century, philosophers like Gottfried Wilhelm Leibniz, through his correspondence with Samuel Clarke (Newton's defender), contended that positing absolute space as a real, independent being multiplied entities beyond what relative relations between bodies required, violating the principle of sufficient reason and rendering space akin to a hidden, god-like medium devoid of empirical warrant.[20] This view framed absolute space as an extravagant hypothesis, preferable only if relative alternatives failed, but ultimately dismissed as an unnecessary complication to the observable order of coexistences. By the 19th century, tensions from electromagnetism intensified these challenges, as James Clerk Maxwell's equations (1860s) necessitated a luminiferous ether as the medium for light propagation at a constant speed, implying a preferred absolute rest frame that clashed with the idea of space's uniform fixity. However, the ether's hypothesized immobility in absolute space raised paradoxes, since planetary motions through it should produce detectable drags or variations in light speed, yet early experiments hinted at no such effects, indirectly eroding confidence in absolute space's role as an unchanging backdrop.[21] These developments, peaking during the Enlightenment and extending into Victorian physics, collectively exposed absolute space and time as increasingly untenable, paving the way for paradigm shifts while relational alternatives, such as Leibniz's, emerged as a key form of opposition.[22]Mathematical Framework
Definitions of Absolute Space
In classical physics, absolute space is defined as a fixed, three-dimensional Euclidean manifold that endures without alteration, independent of any external relations or observers, providing an unchanging arena for the description of physical motions. This conceptual structure posits space as a rigid, homogeneous entity where positions are measured against an immutable grid of coordinates, homogeneous and isotropic, with a preferred frame for absolute rest, though kinematically undetectable.[16] The absoluteness of this space is preserved under Galilean transformations, which connect coordinates between inertial reference frames differing by constant relative velocity . These transformations take the form , , ensuring that spatial distances remain invariant and no phenomena such as length contraction occur, thereby maintaining the fixed geometry of the manifold across frames.[23] Absolute motion within this framework is quantified by the second time derivative of position, , representing acceleration, which proves invariant across all inertial reference frames due to the linearity of Galilean transformations. This independence underscores acceleration as an absolute kinematic quantity, distinguishable from relative velocities that vary between observers. The implications for dynamics are profound: forces acting on bodies are inherently defined relative to this absolute space, permitting the universal applicability of laws like , where the right-hand side captures true, frame-independent acceleration and enables consistent predictions of mechanical behavior irrespective of the observer's motion.[2] This mathematical precision of absolute space received further formalization in the analytic mechanics developed during the 18th and 19th centuries by Joseph-Louis Lagrange and William Rowan Hamilton. Lagrange's Mécanique Analytique (1788) embeds the system's configuration space within the fixed Euclidean manifold, deriving equations of motion through variational principles that presuppose the unchanging spatial structure for generalized coordinates. Hamilton's subsequent reformulation in terms of phase space and the Hamiltonian function (circa 1830s) similarly relies on this absolute backdrop to define canonical momenta and evolve the system deterministically, reinforcing the foundational role of the immutable 3D geometry in classical dynamics.[14]Absolute Time and Dynamics
In Newtonian mechanics, absolute time is defined as a universal parameter that flows equably without regard to anything external, serving as an invariant measure of duration independent of motion, events, or observers.[1] This concept, articulated in the scholium to the definitions in Newton's Philosophiæ Naturalis Principia Mathematica, distinguishes absolute time from relative time, which is sensible and measured by means like the apparent motion of the sun or mechanical clocks.[24] The infinitesimal interval remains constant across all frames, providing a fixed temporal backdrop for physical processes.[14] Absolute time integrates with absolute space in Newtonian dynamics to form a separable 4D spacetime structure, where the full state of a system is specified by position and time , but space and time remain ontologically distinct rather than unified.[14] In this framework, time acts as a scalar parameter parameterizing the evolution of spatial configurations, enabling the laws of motion to describe changes uniformly.[2] For instance, the kinetic energy of a particle of mass moving with velocity relative to absolute space is given by where and , with time serving as the independent variable driving the dynamics.[25] This absolute progression of time underpins classical dynamics, as seen in the example of planetary orbits under gravitational forces, where the uniform flow of allows for precise predictions of elliptical paths and periods without dependence on local observers.[26] In the 19th century, absolute time found refinements in celestial mechanics through Pierre-Simon Laplace's Mécanique Céleste, which extended Newtonian principles to compute long-term solar system stability using uniform temporal parameterization.[27] In thermodynamics, the second law, formulated by Rudolf Clausius, introduces a unidirectional arrow of time through entropy increase as an irreversible process, operating within the framework of absolute time in classical physics.[28]Relativity's Paradigm Shift
Special Relativity
The Michelson-Morley experiment of 1887 sought to detect the Earth's motion through the hypothetical luminiferous ether by measuring differences in the speed of light in perpendicular directions, but yielded a null result, failing to reveal any such motion. This outcome challenged the classical notion of an absolute medium for light propagation and paved the way for a reevaluation of space and time. In 1905, Albert Einstein published his seminal paper "On the Electrodynamics of Moving Bodies," which resolved these issues by formulating special relativity without invoking the ether.[29] Einstein's theory rests on two fundamental postulates: the laws of physics are identical in all inertial reference frames, and the speed of light in vacuum is constant for all observers regardless of the motion of the source or observer.[29] These principles imply the relativity of simultaneity, where events simultaneous in one inertial frame may not be in another moving relative to it, thus eliminating absolute time.[29] To reconcile measurements across frames, Einstein derived the Lorentz transformations, which supersede the Galilean transformations of classical mechanics: where , is the relative velocity, is the speed of light, and primed coordinates denote the moving frame.[29] These equations demonstrate that space and time coordinates mix, rendering both observer-dependent. In 1908, Hermann Minkowski reformulated special relativity geometrically as a four-dimensional spacetime continuum, a flat manifold with the invariant metric This Minkowski spacetime unifies space and time into a single entity, where intervals are absolute but coordinates are relative.[30] Key consequences include time dilation, where the time interval in a frame moving at velocity relative to a stationary observer relates to the proper time by , and length contraction, where the length of an object in the direction of motion is with its proper length.[29] Together, these effects preclude any absolute rest frame, as all inertial frames are equivalent, fundamentally undermining Newton's concepts of absolute space and time.[29]General Relativity
General relativity, formulated by Albert Einstein in 1915, represents a profound departure from the notions of absolute space and time by positing that gravity arises from the curvature of spacetime caused by mass and energy, rendering the geometry dynamic rather than fixed.[31] In this framework, spacetime is not an inert stage but a malleable entity whose structure is determined by the distribution of matter and energy, eliminating any privileged, unchanging backdrop.[31] This theory builds briefly on special relativity as its limit in the absence of gravity, but incorporates the effects of acceleration and gravitation to describe the universe on cosmic scales.[31] Central to general relativity is the equivalence principle, which asserts that the effects of gravity are locally indistinguishable from those of acceleration in a non-inertial frame, such as an elevator in free fall.[31] This principle implies that gravitational fields can be transformed away locally through a suitable choice of coordinates, leading to the requirement of general covariance: the laws of physics must hold in all coordinate systems, without reliance on an absolute space or time.[31] By equating inertial and gravitational mass, it undermines Newton's absolute framework, where gravity acts instantaneously across empty space, and instead suggests that geometry itself encodes gravitational influence.[31] The core of the theory is encapsulated in the Einstein field equations, which relate the curvature of spacetime to the stress-energy content of matter: Here, is the Einstein tensor representing spacetime curvature, derived from the Ricci tensor and scalar, while is the stress-energy tensor describing the distribution of mass, energy, momentum, and stress; is the gravitational constant, and is the speed of light. These equations, first presented in their final form on November 25, 1915, dictate that spacetime curvature responds dynamically to matter-energy, with no underlying absolute metric. The geometry of spacetime is described by the metric tensor , a 4x4 symmetric array that defines distances and intervals locally at each point, varying according to the nearby presence of mass-energy rather than adhering to a universal, flat structure.[31] Unlike absolute space, which provides a fixed arena independent of contents, the metric in general relativity emerges relationally from interactions, ensuring that spatial and temporal measurements are context-dependent.[31] Key implications include the absence of absolute time, manifested in gravitational time dilation where clocks run slower in stronger gravitational fields, as time intervals stretch with the metric component .[31] Similarly, space becomes relational, its configuration shaped by the global distribution of matter, such that distances and simultaneity vary without a rigid grid.[31] These features were empirically validated during the 1919 solar eclipse expeditions led by Arthur Eddington, which measured the deflection of starlight by the Sun's gravity at approximately 1.75 arcseconds, matching general relativity's prediction and contradicting Newtonian expectations.[32]References
- https://en.wikibooks.org/wiki/Special_Relativity/Principle_of_Relativity
