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Absolute space and time
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

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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

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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

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Two spheres orbiting around an axis. The spheres are distant enough for their effects on each other to be ignored, and they are held together by a rope. If the rope is under tension, it is because the bodies are rotating relative to absolute space according to Newton, or because they rotate relative to the universe itself according to Mach, or because they rotate relative to local geodesics according to general relativity.

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

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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

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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

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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

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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

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References and notes

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Absolute space and time is a foundational concept in , introduced by in his 1687 work , positing that space and time exist as absolute, independent entities unaffected by the presence of matter or observers. In the Scholium to the Definitions of the Principia, Newton distinguishes absolute space as remaining "similar and immovable" without relation to anything external, serving as an unchanging backdrop for all physical phenomena, in contrast to relative space, which is a movable dimension or measure arising from the positions of sensible bodies such as the or stars. Similarly, absolute time, also termed "duration," flows equably and uniformly, independent of any external changes or motions, while relative time is an perceptible and approximate measure, like an hour or day, derived from the succession of ideas in the mind or observable celestial cycles. These notions underpin Newton's theory of motion, where absolute motion is defined as the translation of a body from one absolute place to another, detectable through its causes and effects—such as centrifugal forces in a rotating bucket of water—rather than mere changes in relation to surrounding objects. Newton's framework rejected earlier views, including Aristotle's idea of space as a plenum filled with and Descartes' identification of space with bodily extension, instead aligning with a revived atomistic tradition that allowed for void space. Historically, absolute space and time provoked intense debate among Newton's contemporaries and successors; for instance, critiqued them as unnecessary metaphysical entities, arguing instead for relational space and time defined solely by material relations. Despite such opposition, Newton's absolutes dominated Western physics for over two centuries, providing the geometric structure for his laws of motion and universal gravitation, until challenged by Albert Einstein's in the early , which reconceived space and time as intertwined and observer-dependent.

Historical Development

Early Concepts

The concept of space and time in laid foundational intuitions for later absolute notions, emphasizing unchanging frameworks underlying motion and change. , 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. This receptacle implies a stable spatial structure independent of the transient objects it contains, while time is depicted as a "moving image of ," created alongside the to mimic the timeless perfection of the Forms. , 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. For Aristotle, space thus functions as a relational system of places ordered by the 's spherical structure, with time as the measure of change in this plenum, where void has no existence. In medieval , these Greek ideas were synthesized with , positing an absolute divine dimension to space and time. , in his Commentary on Aristotle's Physics, integrated by viewing place and time as real but created entities, subordinate to God's eternal immensity. Space, for Aquinas, reflects divine as an infinite, immaterial expanse encompassing the finite Aristotelian universe, while time derives from mutable creation yet measures motion within God's unchanging eternity. This theological overlay elevated space to an absolute, God-sustained container, bridging Aristotelian relational places with a transcendent framework that ensures cosmic order under . 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 transition, shifted emphasis to in works like , treating space as an isotropic Euclidean arena for describing uniform motion without explicitly invoking absoluteness, yet implicitly assuming a neutral frame for relative velocities. 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.

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. 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. Newton integrated absolute space into his 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. Underlying these scientific formulations were Newton's theological views, where absolute space served as the divine medium for God's . In the General Scholium of the Principia, he asserted that God "endures from to , and is present from to ," constituting duration and space as emanations of His being. Newton further elaborated this in the Opticks (1704), describing infinite space as God's "," 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. articulated this relationalist view in the early , defining space as the order of coexistences among phenomena and time as the order of non-coexistences or successive phenomena. According to Leibniz, these relational orders are ideal abstractions derived from the positions and sequences of bodies, rather than entities subsisting on their own. This perspective came into sharp focus during the 1715–1716 correspondence between Leibniz and , who defended Newton's absolute views. Clarke argued that absolute space was essential to God's immensity, equating infinite space with divine and warning that Leibniz's relationalism would reduce God to a limited, material-dependent being. 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. In the late 19th century, revived and extended relational critiques in his 1883 work The Science of Mechanics, challenging the Newtonian idea of 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 . This "Machian" relationalism emphasized that all motion, including inertial frames, must be empirically grounded in observable cosmic relations, influencing later thinkers like . Philosophically, relationalism resolves paradoxes associated with absolute space, such as the unintelligibility of existing without objects to relate, by deriving spatial and temporal structures entirely from material interactions. It also aligns with empiricist principles, as space and time become verifiable through the relations between events and bodies, eschewing unobservable absolute entities.

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. , 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. 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. , in his analysis of behavior in rotating systems during the late , questioned whether absolute rotation could be confirmed without reference to surrounding , noting that phenomena like centrifugal deviation in a rotating 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. '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 , rather than an unobservable absolute space. Metaphysical objections portrayed absolute space as an occult, superfluous substance that contravened principles of parsimony, such as , by introducing an invisible, infinite entity without explanatory necessity. In the , philosophers like , through his correspondence with (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 and rendering space akin to a hidden, god-like medium devoid of empirical warrant. This view framed absolute space as an extravagant , 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. 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.

Mathematical Framework

Definitions of Absolute Space

In , 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. The absoluteness of this space is preserved under Galilean transformations, which connect coordinates between inertial reference frames differing by constant v\mathbf{v}. These transformations take the form x=xvt\mathbf{x}' = \mathbf{x} - \mathbf{v}t, t=tt' = t, ensuring that spatial distances remain invariant and no phenomena such as occur, thereby maintaining the fixed geometry of the manifold across frames. Absolute motion within this framework is quantified by the second time derivative of position, d2xdt2\frac{d^2 \mathbf{x}}{dt^2}, representing , which proves invariant across all inertial reference frames due to the linearity of 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 F=md2xdt2\mathbf{F} = m \frac{d^2 \mathbf{x}}{dt^2}, where the right-hand side captures true, frame-independent and enables consistent predictions of mechanical behavior irrespective of the observer's motion. This mathematical precision of absolute space received further formalization in the analytic mechanics developed during the 18th and 19th centuries by and . Lagrange's Mécanique Analytique (1788) embeds the system's configuration space within the fixed Euclidean manifold, deriving through variational principles that presuppose the unchanging spatial structure for . Hamilton's subsequent reformulation in terms of 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.

Absolute Time and Dynamics

In Newtonian mechanics, absolute time is defined as a universal parameter tt that flows equably without regard to anything external, serving as an invariant measure of duration independent of motion, events, or observers. This concept, articulated in the scholium to the definitions in Newton's , distinguishes absolute time from relative time, which is sensible and measured by means like the apparent motion of the sun or mechanical clocks. The infinitesimal interval dtdt remains constant across all frames, providing a fixed temporal backdrop for physical processes. 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 x\mathbf{x} and time tt, but space and time remain ontologically distinct rather than unified. In this framework, time acts as a scalar parameter parameterizing the evolution of spatial configurations, enabling the laws of motion to describe changes uniformly. For instance, the kinetic energy of a particle of mass mm moving with velocity v\mathbf{v} relative to absolute space is given by T=12mv2,T = \frac{1}{2} m v^2, where v=vv = |\mathbf{v}| and v=dx/dt\mathbf{v} = d\mathbf{x}/dt, with time tt serving as the independent variable driving the dynamics. This absolute progression of time underpins classical dynamics, as seen in the example of planetary orbits under gravitational forces, where the uniform flow of tt allows for precise predictions of elliptical paths and periods without dependence on local observers. 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. 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.

Relativity's Paradigm Shift

Special Relativity

The Michelson-Morley experiment of 1887 sought to detect the Earth's motion through the hypothetical luminiferous by measuring differences in the 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 and time. In 1905, published his seminal paper "On the Electrodynamics of Moving Bodies," which resolved these issues by formulating without invoking the . 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. These principles imply the , where events simultaneous in one inertial frame may not be in another moving relative to it, thus eliminating absolute time. To reconcile measurements across frames, Einstein derived the Lorentz transformations, which supersede the Galilean transformations of : x=γ(xvt),t=γ(tvxc2),x' = \gamma (x - vt), \quad t' = \gamma \left( t - \frac{vx}{c^2} \right), where γ=11v2c2\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}
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