Length contraction
George Francis FitzGerald proposed a physical shortening of objects in 1889 to explain why the Michelson, Morley experiment found no evidence of Earth's motion through the stationary aether. Hendrik Antoon Lorentz refined this idea in 1892, suggesting that intermolecular forces behaved like electromagnetic ones to cause this contraction. Oliver Heaviside had previously derived how electrostatic fields deform into what became known as the Heaviside-Ellipsoid in 1888. Joseph Larmor developed a model in 1897 where all forces were considered electromagnetic origins for length contraction. Henri Poincaré showed in 1905 that electromagnetic forces alone could not explain electron stability without introducing non-electric binding forces called Poincaré stresses. Lorentz believed these contractions represented actual physical compression of atoms rather than a change in space itself. He expected measurable optical effects such as double refraction or torques on charged condensers moving at angles to the aether. The Trouton, Noble experiment and Rayleigh-Brace experiments failed to validate his theoretical expectations regarding these compressive strains.
Albert Einstein published his theory of special relativity in 1905 and removed the ad hoc character from the contraction hypothesis entirely. He declared the concept of a stationary aether superfluous along with any absolutely stationary space. Einstein proposed that Lorentz's transformation apply to both electromagnetism and mechanics simultaneously. Hermann Minkowski later gave geometrical interpretation to all relativistic effects by introducing four-dimensional spacetime. Einstein argued in 1911 that length contraction was not simply the product of arbitrary definitions concerning clock regulations. He presented a thought experiment involving two rods of proper length L0 moving in opposite directions along an axis considered at rest. Endpoints A'A" met at point A while B'B" met at point B. Einstein pointed out that distance A*B* is shorter than either A'B' or A"B". This demonstrated that length contraction occurs objectively when one rod is brought to rest relative to that axis. The principle of relativity requires laws of nature to be invariant across inertial reference frames regardless of motion.
The deviation between measurements in all inertial frames follows formulas for Lorentz transformation and time dilation. Proper length remains unchanged and always denotes the greatest length of an object measured in its own rest frame. An observer in another inertial reference frame measures a shorter length contracted by factor gamma. Gamma equals one divided by the square root of one minus v squared over c squared where v is relative velocity and c is speed of light. At thirty million miles per hour which equals zero point zero four four seven times c, contracted length reaches ninety-nine point nine percent of rest length. At ninety-five million miles per hour equaling zero point one four one times c, length stays at ninety-nine percent. As magnitude of velocity approaches speed of light, effect becomes prominent. Symmetry exists because if a rod rests in frame S it has proper length there but contracts in frame S'. If rod rests in S', it has proper length there but contracts in S. Minkowski diagrams illustrate this symmetry geometrically as rotation in four-dimensional spacetime. Poincaré transformations are affine transformations between alternative Cartesian coordinate charts on Minkowski spacetime corresponding to states of inertial motion. Lorentz transformations form isotropy group of self-isometries of spacetime playing same role as rotations do in Euclidean geometry.
Indirect confirmations exist through muon decay despite extremely short lifespans preventing surface travel from atmosphere thickness measured in Earth's reference frame. Muons reach ground only because time slows down for them according to time dilation or because atmosphere contracts in their own frame. Heavy ions spherical when at rest assume pancake or flat disk forms traveling near speed of light. Results from particle collisions require increased nucleon density due to length contraction to be explained correctly. Ionization ability of electrically charged particles with large relative velocities exceeds pre-relativistic expectations. Time interaction diminishes ionizing power yet relativistic contraction increases electrical field strength normal to line of motion. Synchrotrons inject relativistic electrons into undulators generating synchrotron radiation where undulator contracts in electron proper frame leading to increased frequency. Laboratory frame measurements apply relativistic Doppler effect to explain extremely small wavelengths of undulator radiation. Direct experimental confirmation remains hard because objects of considerable extension cannot accelerate to required speeds while atomic particles have spatial extensions too small for direct measurement.
André-Marie Ampère demonstrated parallel wires carrying currents in same direction attract one another back in 1820. Magnetic force on moving charge next to current-carrying wire results from relativistic motion between electrons and protons. In electrons' frame of reference, moving wire contracts slightly causing protons of opposite wire to become locally denser. Electrons in opposite wire move as well but do not contract as much resulting in apparent local imbalance. Moving electrons in one wire attract extra protons in other wire creating magnetic attraction. Reverse perspective shows static proton sees electrons moving and contracted producing same imbalance. Electron drift velocity reaches order of a meter per hour yet force between electron and proton remains enormous enough that even slow speed causes significant effects through relativistic contraction. Effect applies to magnetic particles without current replacing current with electron spin. This mechanism explains how magnetism emerges fundamentally from electric forces combined with relative motion and length contraction.
Roger Penrose and James Terrell wrote about visual effects now called Terrell rotation in 1959 clarifying earlier confusion. Lorentz erroneously claimed in 1922 that contractions could be photographed directly while George Gamow illustrated bicycles as only foreshortened in Mr Tompkins in Wonderland illustrations. A paper with correct appearance published in 1924 remained widely unread until Terrell's work clarified difficulties. Length contraction refers to measurements made at simultaneous times according to coordinate system unlike photographs taken from distance. Victor Weisskopf popularized result showing moving objects generally do not appear length contracted on photograph. For small angular diameter, moving sphere remains circular but appears rotated instead. This kind of visual rotation effect is called Penrose-Terrell rotation. Paradoxes like ladder paradox and Bell's spaceship paradox occur due to superficial application of contraction formula. Ehrenfest paradox proves concept of rigid bodies incompatible with relativity reducing applicability of Born rigidity. Co-rotating observer finds geometry becomes non-Euclidean rather than Euclidean as expected from classical mechanics assumptions.
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Common questions
Who proposed length contraction in 1889 to explain the Michelson Morley experiment results?
George Francis FitzGerald proposed a physical shortening of objects in 1889 to explain why the Michelson Morley experiment found no evidence of Earth's motion through the stationary aether. Hendrik Antoon Lorentz refined this idea in 1892 by suggesting that intermolecular forces behaved like electromagnetic ones to cause this contraction.
When did Albert Einstein publish his theory of special relativity and how did it change the concept of length contraction?
Albert Einstein published his theory of special relativity in 1905 and removed the ad hoc character from the contraction hypothesis entirely. He declared the concept of a stationary aether superfluous along with any absolutely stationary space and proposed that Lorentz's transformation apply to both electromagnetism and mechanics simultaneously.
What is the formula for gamma used to calculate length contraction at specific velocities?
Gamma equals one divided by the square root of one minus v squared over c squared where v is relative velocity and c is speed of light. At thirty million miles per hour which equals zero point zero four four seven times c, contracted length reaches ninety-nine point nine percent of rest length.
How does length contraction explain magnetic attraction between parallel wires carrying currents?
Magnetic force on moving charge next to current-carrying wire results from relativistic motion between electrons and protons. In electrons' frame of reference, moving wire contracts slightly causing protons of opposite wire to become locally denser and creating an apparent local imbalance that attracts extra protons.
Why do photographs of objects moving near the speed of light not show direct length contraction according to Roger Penrose and James Terrell?
Length contraction refers to measurements made at simultaneous times according to coordinate system unlike photographs taken from distance. Victor Weisskopf popularized result showing moving objects generally do not appear length contracted on photograph because a kind of visual rotation effect called Penrose-Terrell rotation occurs instead.