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Undid revision 311161695 by Martin Hogbin (talk)No unreferenced opinon found here. Use Talk page
Revert to Martin's version. This does not belong here, or anywhere, for what matters.
Line 1,296: Line 1,296:
|volume=29
|volume=29
|doi=10.1103/PhysRevLett.29.189 }}
|doi=10.1103/PhysRevLett.29.189 }}
⚫
</ref>
</ref> Mathematically, comparison of two lengths ℓ<sub>1</sub>, ℓ<sub>2</sub> with times-of-transit of light, ''t''<sub>1</sub>, ''t''<sub>2</sub> may be expressed as the ratio:

::<math> \frac {\ell_1}{\ell_2} = \frac {c\ t_1}{c\ t_2} = \frac {t_1}{t_2} \ , </math>

which is independent of the speed of light ''c'', so long as the same speed of light is realized while measuring both times-of-transit. As an example, if the time ''t''<sub>2</sub> in the above equation is selected as {{nowrap begin}} ''t''<sub>2</sub> = 1 <big>/</big> 299 792 458 s,{{nowrap end}} and the measurement is done in ‘vacuum’, then ℓ<sub>1</sub> is determined in metres. It is apparent that the determination of ℓ<sub>1</sub> in units of metres depends in no way at all upon the defined value for the conversion factor ''c'', but is determined entirely by the committee's choice of the standard time interval {{nowrap begin}} ''t''<sub>std</sub> = 1 <big>/</big> 299 792 458 s{{nowrap end}}.

====Measuring the speed of light====
If one wishes to measure the speed of light, not just use the SI system with its defined relationship between the metre and the speed of light, that can be done by introducing a unit of length other than the metre, for example the wavelength of an atomic transition, as was done in the earlier definition of the metre before 1983:<ref name=timeline>[http://www.nist.gov/mel/ped/museum-timeline.cfm NIST timeline of definitions of the metre]</ref>

<blockquote>"On October 14, 1960 the Eleventh General Conference on Weights and Measures redefined the International Standard of Length as 1,650,763.73 vacuum wavelengths of light resulting from unperturbed atomic energy level transition 2p<sub>10</sub> 5d<sub>5</sub> of the krypton isotope having an atomic weight of 86. The wavelength is

::λ = 1 m / 1,650,763.73 = 0.605,780,211 µm

At different times some national laboratories used light sources other than krypton 86 as length standards. Mercury 198 and cadmium 114 were among these and they were accepted by the General Conference as secondary length standards."</blockquote>

Because a length such as the wavelength of an atomic transition is determined from the transit time using the relation:

::<math> \ell = c\ t \ , </math>

where ''c'' is the speed of light to be measured, the speed of light can be determined in units of wavelengths per second by [[interferometry|counting interference fringes]]<ref name=Hariharan>
{{cite book
|title=Optical interferometry
|author=P. Hariharan
|url=http://books.google.com/books?id=EGdMO3rfVj4C&pg=PA105
|pages=105 ''ff''
|chapter=Measurement of length
|isbn=0123116309
|year=2003
|edition=2nd
|publisher=Academic Press
⚫
}}</ref>
and dividing by the measured period of the transition. This speed of light in terms of an independent length standard would be ''not'' an exactly known value, set by definition, but a measured value subject to experimental error.


==See also==
==See also==

Revision as of 01:40, 1 September 2009

For other uses, see Speed of light (disambiguation).
"Lightspeed" redirects here. For other uses, see Lightspeed (disambiguation).
Sunlight takes approximately 500 seconds to reach Earth.
Speed of light in different units
  metres per second 299,792,458 (exact)
  km per second 299,792.458 (exact)
  km per hour ≈ 1,079,252,848
  miles per second ≈ 186,282
  miles per hour ≈ 670,616,629
Approximate length of time for light to travel...
 One foot 1.0 nanoseconds
 One metre 3.3 nanoseconds
 One km 3.3 microseconds
 One mile 5.4 microseconds
 To Earth from geostationary orbit 0.12 seconds
 The length of Earth's equator 0.13 seconds
 To Earth from the moon 1.3 seconds
 To Earth from the sun 8.3 minutes
 To Earth from Alpha Centauri 4.4 years
 Across the Milky Way 100,000 years

The speed of light "c" is a fundamental constant of nature. It is the speed at which light and all electromagnetic radiation travel in space or vacuum. After much debate and scientific study, light is now known to travel at approximately 300,000 km per second. It is of vital importance in the understanding and study of relativity, spacetime, astronomy and space travel.

For much of human history the nature of light, including whether it was instanteneous or simply travelled very quickly, was unknown. By the 11th century many scientists had realised that light had a finite speed but it was not until the 17th century that Ole Rømer demonstrated this by observing small differences in the apparent orbital period of one of Jupiter's moons. Using this data, Christiaan Huygens estimated the speed of light to be about 220,000 km per second. Since then, scientists have devised more sophisticated techniques to improve the precision of measurement and, by the mid-20th century, the speed of light was known to be approximately 299,792,458 metres per second. For technical reasons in 1983, the metre was redefined using this value as a conversion factor. This had the effect of 'fixing' c at exactly 299,792,458 metres per second in the International System of Units.

In 1905, Albert Einstein's special theory of relativity revealed that the speed of light is an important constant connecting space and time in the unified structure of spacetime. As such, it defines the conversion between mass and energy[1] and is an upper bound on the speed at which matter and information can travel.[2][3] It is the speed of travel of all electromagnetic radiation in free space,[4] and is believed to be the speed of gravitational waves.[5][6] In an inertial frame, light in vacuum always travels at c, however, when light passes through a transparent medium, such as glass or air, its speed is less. The ratio between the speed of light in vacuum and the speed of light in a medium is called the refractive index of the medium.

Numerical value, notation and units

The speed of light is a dimensional constant, so its numerical value depends upon the system of units used. In the SI system, the metre is defined as the distance light travels in vacuum in 1⁄299792458 of a second. The effect of this definition is to fix the speed of light in vacuum at exactly 299792458 m/s.[7][8][9]

The symbol c for "constant" or the Latin celeritas (meaning "swiftness")[10] is used for the speed of light in vacuum, and in this article c is used exclusively this way. Some authors, however, use c for the speed of light in any material medium, and c0 for the speed of light in vacuum.[11] This subscripted notation, which is endorsed in official SI literature,[12] has the same form as other related constants; namely μ0, ε0 and Z0.

In branches of physics in which the speed of light plays an important part, such as in relativity, it is common to use a system of units known as natural units in which c = 1.[13] Thus, no symbol for the speed of light is required.

Fundamental importance in physics

Light as electromagnetic radiation

See also: Electromagnetic spectrum

Light is a form of electromagnetic radiation. In the theory of classical electromagnetism such radiation is described by the electromagnetic wave equation, which is derived from Maxwell's equations. According to this theory, the speed of light in vacuum is related to the electric constant ε0 and the magnetic constant μ0 by the equation c02 = 1/(ε0μ0) in SI units.[14] Thus, as the value of the magnetic constant is fixed in SI units by definition, the value of the electric constant is also fixed. In Gaussian units, the speed of light fixes the ratio between electrostatic and electromagnetic units.

A more complete theory of light that describes the interaction of photons with matter is given by quantum electrodynamics (QED). Here the speed of light enters the theory via the dimensionless fine structure constant α.[15]

Constant speed in inertial frames

See also: Introduction to special relativity and Special relativity

The speed of light has been shown experimentally to be independent of the motion of the source.[16][17] It has also been confirmed by the Michelson–Morley experiment and other experiments that the two-way speed of light (for example from a source to a mirror and back again) is constant.[16][18][19][20]

It is not possible, however, to measure the one-way speed of light (for example from a source to a distant detector) without some convention as to how clocks at the source and detector should be synchronized.[16] Einstein (who was aware of this fact) postulated that the speed of light in an inertial frame should be taken as constant in all cases. That postulate is fundamental to the theory of special relativity.[21][22] Although the speed of propagation is independent of motion of the source, the observed frequency can change due to the Doppler effect.

In general relativity the concepts of 'distance', 'time', and therefore 'speed' are not always unambiguously defined due to the curvature of spacetime caused by gravitation.[23] Similarly measurements of the speed of light made in non-inertial frames may give values other than c depending on how distances and times are defined.

Spacetime constant

See also: Spacetime, Minkowski space, and Lorentz group
Fusion of deuterium with tritium creating helium-4, freeing a neutron, and releasing 17.59 MeV of energy by conversion of mass in accord with E = mc2.[24]

In Einstein's theory of special relativity space and time are viewed as a four dimensional unification of space and time, known as spacetime,[25] with c playing the fundamental role of a conversion factor between the units of space and time,[26] and also between mass and energy according to the famous mass-energy equation E = mc2.[27]

The finite speed of light in relativity leads to some counter-intuitive consequences, which include length contraction, time dilation and the relativity of simultaneity, this last item contradicting the classical notion that the duration of the time interval between two events is equal for all observers.

In Einstein's general theory of relativity, c is still an important constant of spacetime. This spacetime is curved by the presence of matter and energy causing gravitation.[28] Disturbances in this curvature, including gravitational waves, propagate at the speed of light.[29][30]

Causality and information transfer

See also: Causal contact, Tachyonic antitelephone, and Horizon problem
A light cone defines locations that are in causal contact and those that are not.

According to the theory of special relativity, causality would be violated if information could travel faster than c in some reference frame. In some other reference frames, the information would be received before it had been sent, so the "effect" could be observed before the "cause". Such a violation of causality has never been recorded,[16] and would lead to paradoxes.[31]

Information propagates to and from a point forming regions defined by a light cone. The interval AB in the diagram to the right is "time-like" (that is, there is a frame of reference in which event A and event B occur at the same location in space, separated only by their occurring at different times, and if A precedes B in that frame then A precedes B in all frames: there is no frame of reference in which event A and event B occur simultaneously). Thus, it is hypothetically possible for matter (or information) to travel from A to B, so there can be a causal relationship (with A the "cause" and B the "effect"). In other words, c represents the maximum speed at which matter, energy, or information can be transmitted.

On the other hand, the interval AC in the diagram to the right is "space-like" (that is, there is a frame of reference in which event A and event C occur simultaneously, separated only in space; see simultaneity). In some frames A precedes C (as shown), but in others C precedes A. Therefore there can be no causal connection between A and C, and in particular it is not possible for any matter (or information) to travel from A to C or from C to A.[32]

Composition of velocities

See also: Velocity addition formula and Fizeau–Foucault apparatus

If two cars approach each other from opposite directions, each traveling at a speed of 50 km/h relative to the road surface, according to intuitive Galilean relativity, one expects that an observer in one car will measure the speed of approach of the other car as 50 + 50 = 100 km/h. However, as speeds increase, the simple addition of speeds becomes less accurate. Two spaceships approaching each other, each traveling at 90% of the speed of light in opposite directions relative to some third observer, would not measure each other as approaching at 90% + 90% = 180% the speed of light; instead they each measure the other as approaching at slightly less than 99.5% the speed of light. This last result is given by the velocity-composition formula[33]

where v1 and v2 are the velocities of the spaceships as measured by the third observer, and u is the measured velocity of either spaceship as observed by the other. This reduces to u = v1 + v2 for sufficiently small values of v1 and v2 (such as those typically encountered in common daily experiences) as the term (v1·v2)/c2 approaches zero, reducing the denominator to 1.

If one of the two velocities v in the above formula (or both) is c, the final result is c, as is expected if the speed of light is the same in all inertial reference frames. Another important result is that this formula never returns a value greater than c: this is consistent with c being the maximum possible speed.

Light and photons

Main articles: Light and Photon
See also: Virtual particle and Force carrier

Quantum field theory reflects not only the wave aspects of light, but the wave-particle duality of light. The electromagnetic forces between charged particles are seen as mediated by exchange of photons (messenger particles). One early argument for photons was Einstein's Nobel Prize winning explanation of the photoelectric effect in terms of a particulate model of light.[34]

At present, the rest mass of the photon is taken to be zero, with an experimental upper bound of about 10−57 g.[35] This is assuming that a hypothetically massive photon is described by Proca theory.[36]. In case of a photon mass generated by a Higgs mechanism, the experimental upper limit is less sharp, m ≤ 10−14 eV[36] (equivalent to of the order of 10−47 g).

If the photon had mass, one result would be that the speed of light would not be constant over all frequencies.[37]

Cosmology and quantum gravity

See also: Physical cosmology, Primordial fluctuations, Cosmological constant, and Variable speed of light
See also: Quantum gravity, Graviton, Planck scale, and Doubly-special relativity

Some scientists have questioned why the fundamental constants of nature, including the speed of light, have the values they do, and whether they are changing as the universe evolves.[38][39][40] These questions remain an interest of on-going research.[41][42][43][44][45][46]

Others have suggested that the speed of light may exhibit a small dispersion—that is, different frequencies may travel at slightly different velocities.[47][48][49] However, to date, such variations, if any, are smaller than experimental errors of observation—the measured speed of electromagnetic radiation is the same for different frequencies to within very stringent experimental limits.[50][51][52]

Light in transparent media

Refractive index and refraction

See also: Refractive index and Snell's law

When light travels through a transparent material, it travels more slowly that it does through vacuum. This is due to the interaction of the light with the electrons bound to the atoms in the material.[53] The refractive index of a transparent material indicates how much slower light propagates in that medium than in a vacuum, being the ratio of c to the speed of light in the material. The refractive index of a material is often taken as a constant, but in some materials it may depend on the light's frequency, intensity, polarization, or direction of propagation. The refractive index in air is only slightly larger than one.[54] Denser media, such as water and glass, have refractive indices of around 1.3 and 1.5 respectively for visible light. Diamond has a refractive index of about 2.4.

Classically, when an electromagnetic wave meets the surface of a dielectric material at an angle, the leading edge is slowed while the trailing edge continues normally. This causes the wave to change direction. This is called refraction and the change in direction may be calculated from the refractive index using Snell's law.[55]

Dispersion

See also: Dispersion (optics), Electric susceptibility, and Permittivity
File:PrismAndLight.jpg
The light passing through this prism demonstrates refraction and, by the splitting of white light into a spectrum of colours, dispersion.

The dependence of the speed of light in a material on its frequency is known as dispersion. When a light pulse comprised of multiple frequencies passes through transparent materials, the speed of light is characterized by two speeds: the phase velocity and the group velocity. The phase velocity of light may be found from knowledge of the frequency-dependent refractive index:

where εr is the material's relative permittivity, and μr is its relative permeability.

The group velocity of the wave is the speed at which the envelope of the pulse travels through the medium, and is dependent on the frequency content of the pulse as well as the properties of the medium. A wave with different group and phase velocities is said to undergo dispersion.

When light enters materials its energy is absorbed. In the case of transparent materials (dielectrics) this energy is quickly re-radiated. However, this absorption and re-radiation introduces a delay. As light propagates through dielectric material it undergoes continuous absorption and re-radiation. Therefore when the speed of light in a medium is said to be less than c, this should be read as the speed of energy propagation at the macroscopic level. At an atomic level, electromagnetic waves always travel at c in the empty space between atoms. Two factors influence this slowing; stronger absorption leading to shorter path length between each re-radiation cycle and longer delays. The slowing is therefore the product of these two factors. This reduction in speed is also responsible for bending of light at an interface between two materials with different refractive indices, a phenomenon known as refraction.

General media

In real materials the current and charge densities appearing in Maxwell's equations are determined by the way charges respond to the electromagnetic fields. One approach to describing this behavior is the calculation of constitutive equations, which describe how charges behave within the medium, usually using a linear approximation. (Ohm's law is an example.) In simplest form, the constitutive equations replace the electric constant and magnetic constant by the electric permittivity and magnetic permeability of the medium. However, nonlinear behavior also occurs, as in ferroelectric materials, for example. A consequence of the charge response to fields is that the speed of light may become dependent upon field amplitudes, polarization, direction of propagation, and frequency. One field concerned with the calculation of these relationships is condensed matter physics.

Slow light

Main article: Slow light

Certain materials have an exceptionally high group index and a correspondingly low group velocity for light waves. In 1999, a team of scientists led by Lene Hau were able to slow the speed of a light pulse to about 17 m/s;[56] in 2001, they were able to momentarily stop a beam.[57]

In 2003 scientists at Harvard University and the Lebedev Physical Institute in Moscow, succeeded in completely halting light by directing it into a Bose–Einstein condensate of the element rubidium, the atoms of which, in Lukin's words, behaved "like tiny mirrors" due to an interference pattern in two "control" beams.[58][59]

Faster-than-light observations and experiments

Main article: Faster-than-light
See also: Scharnhorst effect and Hartman effect
The blue glow in this "swimming pool" nuclear reactor is Čerenkov radiation, emitted as a result of electrons traveling faster than the speed of light in water.

It is generally considered that it is impossible for any information or matter to travel faster than c, because it would travel backwards in time relative to some observers.[60] However, there are many physical situations in which speeds greater than c are encountered.

Some of these situations involve entities that actually travel faster than c in a particular reference frame but none involves either matter, energy, or information traveling faster than the speed of light in vacuum.

It is possible for the group velocity of light to exceed c[61][62] and in an experiment in 2000 laser beams traveled for extremely short distances through caesium atoms with a group velocity of 300 times c.[63] It is not, however, possible to use this technique to transfer information faster than c since the velocity of information transfer depends on the front velocity, which is always less than c.[64]

If a laser is swept across a distant object, the spot of light can easily be made to move at a speed greater than c.[65] Similarly, a shadow projected onto a distant object can be made to move faster than c.[66] In neither case does any matter or information travel faster than light.

In some interpretations of quantum mechanics, certain quantum effects may be transmitted at speeds greater than c. For example, the quantum states of two particles can be entangled. Until the particles are observed, they exist in a superposition of two quantum states. If the particles are separated and one of them is observed to determine its quantum state then the quantum state of the second particle is determined automatically and faster than a light signal could travel between the two particles. However, it is impossible to control which quantum state the first particle will take on when it is observed, so no information can be transmitted in this manner.

Another prediction of faster-than-light speeds occurs for quantum tunneling and is called the Hartman effect.[67][68] However, no information can be sent using these effects.[69]

Closing speeds and proper speeds are examples of calculated speeds that may have value in excess of c but that do not represent the speed of an object as measured in a single inertial frame.

So-called superluminal motion is seen in certain astronomical objects,[70] such as the jets of radio galaxies and quasars. However, these jets are not moving at speeds in excess of the speed of light: the apparent superluminal motion is a projection effect caused by objects moving near the speed of light and at a small angle to the line of sight.

Cherenkov radiation
Main article: Cherenkov radiation

It is possible for shock waves to be formed with electromagnetic radiation.[71][72] If a charged particle travels through an insulating medium faster than the speed of light in that medium (but always slower than the speed of light in vacuum) then electromagnetic radiation is emitted which is analogous to a sonic boom and is known as Čerenkov radiation.

Galaxies moving faster than light
See also: Metric expansion of space, Hubble's Law, Observable universe, and Cosmological horizon

In models of the expanding universe, the further things are from Earth, the faster they move away from us. This movement is not considered to be a straightforward travel, like a rocket for example, but a movement due to the expansion of space itself. This expansion moves distant objects away from us faster and faster the further away they are. At a boundary called the Hubble sphere, the recessional velocity is the speed of light.

Practical effect of the finite speed of light

As light propagates down the telescope, the telescope moves, so observing the light requires a tilt to the telescope that depends on c. The apparent angle of the star φ differs from its true angle θ.

The speed of light plays an important part in many modern sciences and technologies. Radar systems measure the distance to a target by measuring the time taken for an echo of the light pulse to return. Similarly, a global positioning system (GPS) receiver measures its distance to satellites based on how long it takes for a radio signal to arrive from the satellite. The distances to the moon, planets, and spacecraft are determined by measuring the round-trip travel time.

Another effect of the finite speed of light is stellar aberration. Suppose we look at a star with a telescope idealized as a narrow tube. The light enters the tube from a star at angle θ and travels at speed c taking a time h/c to reach the bottom of the tube, where our eye detects the light. Suppose observations are made from Earth, which is moving with a speed v. During the transit of the light, the tube moves a distance vh/c. Consequently, for the photon to reach the bottom of the tube, the tube must be inclined at an angle φ different from θ , resulting in an apparent position of the star at angle φ.

In astronomy beyond the solar system, distances are often measured in light-years, the distance light travels in a year.

In electronic systems, despite their small size, the speed of light can become a limiting factor in their maximum speed of operation.[73][74][75]

Terrell rotation

Objects passing rapidly by an observer will be measured to have shrunk along the line of relative motion due to Lorentz contraction, but they will be actually seen as being rotated. This is due to the differences in time that it takes light to reach the eye of the observer from different parts of the object.[76][77] This effect is known as Terrell rotation.

Speed of light in astronomy

The relative sizes and separation of the Earth–Moon system are shown to scale above. The beam of light is depicted traveling between the Earth and the Moon in the same time it actually takes light to scale the real distance between them: 1.255 seconds at its mean orbital distance (surface to surface). The light beam helps provide the sense of scale of the Earth-Moon system relative to the Sun, which is 8.28 light-minutes away (photosphere to Earth surface).

The speed of light is particularly important in astronomy. Due to the vast distances involved it can take a very long time for light to travel from its source to Earth. For example, it takes 13 billion years for light to travel to Earth from the faraway galaxies viewed in the Hubble Ultra Deep Field images. Those photographs, taken today, capture images of the galaxies as they appeared 13 billion years ago (near the beginning of the universe). The fact that farther-away objects appear younger (due to the finite speed of light) is crucial in astronomy, allowing astronomers to infer the evolution of stars, galaxies, and the universe itself.

Astronomical distances are sometimes measured in light-years, the distance light travels in one year. A light‑year is around 9 trillion km, 6 trillion miles, or 0.3 parsecs. Next to the Sun, the closest star to Earth, Proxima Centauri, is around 4.2 light‑years away.[78]

Redshift of spectral lines in the optical spectrum of a supercluster of distant galaxies (right), as compared to that of the Sun (left).

Doppler effect

The Doppler effect for electromagnetic waves such as light is of great use in astronomy and results in either a so-called redshift or blue shift. It has been used to measure the speed at which stars and galaxies are approaching or receding from us, that is, the radial velocity. This is used to detect if an apparently single star is, in reality, a close binary and even to measure the rotational speed of stars and galaxies.

History

Ancient, medieval, and early modern speculation

Until relatively recent times, it was not known whether the speed of light was infinite. The debate began in ancient Greece. Empedocles maintained that light was something in motion, and therefore there had to be some time elapsed in traveling. Aristotle said that, on the contrary, "light is due to the presence of something, but it is not a movement".[79] Euclid and Ptolemy advanced the emission theory of vision, which claimed light was emitted from the eye, thus enabling sight. Using that theory, Heron of Alexandria advanced the argument that the speed of light must be infinite, since distant objects such as stars appear immediately upon opening the eyes.

Early Muslim philosophers initially agreed with the Aristotelian view of the speed of light being infinite. In 1021, Iraqi physicist Alhazen (Ibn al-Haytham) published the Book of Optics, in which he used experiments related to the camera obscura to support the intromission theory of vision, which claimed that light moves from an object into the eye.[80] This led to Alhazen proposing that light must therefore have a finite speed,[79][81][82] and that the speed of light is variable, with its speed decreasing in denser bodies.[82][83] He argued that light is a "substantial matter", the propagation of which requires time "even if this is hidden to our senses".[84] This debate continued in Europe and the Middle East throughout the Middle Ages.

Also in the 11th century, Abū Rayhān al-Bīrūnī agreed that light has a finite speed, and observed that the speed of light is much faster than the speed of sound.[85] Roger Bacon argued that the speed of light in air was not infinite, using philosophical arguments backed by the writing of Alhazen and Aristotle.[86][87] In the 1270s, Witelo considered the possibility of light traveling at infinite speed in a vacuum but slowing down in denser bodies.[88] A comment on a verse in the Rigveda by the 14th century Indian scholar Sayana[89] may be interpreted as suggesting an estimate for the speed of light that is in good agreement with its actual speed. In 1574, the Ottoman astronomer and physicist Taqi al-Din concluded that the speed of light is constant, but variable in denser bodies, and suggested that it would take a long time for light from the stars, which are very distant, to reach the Earth.[90]

In the early 17th century, Johannes Kepler believed that the speed of light was infinite since empty space presents no obstacle to it. René Descartes argued that if the speed of light were finite, the Sun, Earth, and Moon would be noticeably out of alignment during a lunar eclipse. Since such misalignment had not been observed, Descartes concluded the speed of light was infinite. Descartes speculated that if the speed of light was found to be finite, his whole system of philosophy might be demolished.[79]

First attempts to measure the speed of light

In 1629, Isaac Beeckman proposed an experiment in which a person would observe the flash of a cannon reflecting off a mirror about one mile (1.6 km) away. In 1638, Galileo Galilei proposed an experiment, with an apparent claim to having performed it some years earlier, to measure the speed of light by observing the delay between uncovering a lantern and its perception some distance away. He was unable to distinguish whether light travel was instaneous or not, but concluded that if it weren't, it must nevertheless be extraordinarily rapid.[91][92] Galileo's experiment was carried out by the Accademia del Cimento of Florence in 1667, with the lanterns separated by about one mile (1.6 km), but no delay was observed. Based on the modern value of the speed of light, the actual delay in this experiment would be about 11 microseconds. Robert Hooke explained the negative results as Galileo had by pointing out that such observations did not establish the infinite speed of light, but only that the speed must be very great.

Astronomical techniques

Rømer's observations of the occultations of Io from Earth

The first quantitative estimate of the speed of light was made in 1676 by Ole Christensen Rømer, who was studying the motions of Jupiter's moon, Io, with a telescope. It is possible to time the orbital revolution of Io because it enters and exits Jupiter's shadow at regular intervals (at points C and D in the diagram at right). Rømer observed that Io revolved around Jupiter once every 42.5 hours when Earth was closest to Jupiter (at H). He also observed that, as Earth and Jupiter moved apart, (as from L to K), Io's exit from the shadow would begin progressively later than predicted. He realized that these exit "signals" took longer to reach Earth as a result of the extra time it took for light to cross the extra distance between the moving planets. The opposite is the case when they are approaching (as from F to G). Rømer observed 40 orbits of Io when Earth was approaching Jupiter to be 22 minutes shorter than 40 orbits of Io when Earth was moving away from Jupiter.[93] On the basis of those observations, Rømer concluded that it took light 22 minutes to cross the distance the Earth traversed in 80 orbits of Io.[93] This means that in traveling from L to K and F to G, whereas the earth took 80 periods of Io's orbits (42.5 hours), the light only took 22 minutes. This corresponds to a ratio between the speed of light and the speed at which the Earth travels in its orbit around the sun of 9,300. The modern value of the ratio is about 10,100.

Around the same time, the astronomical unit (roughly, the Earth-to-Sun distance) was estimated to be about 140 million kilometres (87 million miles). The astronomical unit and Rømer's time estimate were combined by Christiaan Huygens, who estimated the speed of light to be 1,000 Earth diameters per minute, based on having misinterpreted Rømer's value of 22 minutes to mean the time it would take light to cross the diameter of the orbit of the Earth.[93] This is about 220,000 kilometres per second (136,000 miles per second), 26% lower than the currently accepted value, but still very much faster than any physical phenomenon then known.[94]

Isaac Newton also accepted the finite speed. In his 1704 book Opticks he reports the value of 16.6 Earth diameters per second (210000 km/s). The same effect was subsequently observed by Rømer for a "spot" rotating with the surface of Jupiter. Later observations also showed the effect with the three other Galilean moons, where it was more difficult to observe, thus laying to rest some further objections that had been raised.

In 1728, James Bradley deduced that starlight falling on the Earth should appear to come from a slight angle, which could be calculated by comparing the speed of the Earth in its orbit to the speed of light. This "aberration of light", as it is called, was observed to be about 1/200 of a degree. Bradley calculated the speed of light as about 298000 km/s (186000 mi/s).

Earth-bound techniques

See also: Fizeau–Foucault apparatus
Diagram of the Fizeau apparatus

The first successful entirely earthbound measurement of the speed of light was carried out by Hippolyte Fizeau in 1849. Fizeau's experiment was conceptually similar to those proposed by Beeckman and Galileo. A beam of light was directed at a mirror 8 km away. On the way from the source to the mirror, the beam passed through a rotating cog wheel. At a certain rate of rotation, the beam could pass through one gap on the way out and another on the way back. But at slightly higher or lower rates, the beam would strike a tooth and not pass through the wheel. Knowing the distance to the mirror, the number of teeth on the wheel, and the rate of rotation, the speed of light could be calculated. Fizeau reported the speed of light as 313000 km/s. Leon Foucault improved on Fizeau's method by replacing the cogwheel with a rotating mirror. Foucault's estimate, published in 1862, was 298000 km/s.

Modern methods

Electromagnetic standing waves in a cavity. Sinusoidal waves at the top have larger frequencies than below and are shifted upward for clarity. The conductive walls require the nodes of the standing wave to be at the wall surfaces, so the allowed wavelengths are: λ/2 = W, λ = W, 3λ/2 = W where W = width of cavity.

During World War II, the development of the cavity resonance wavemeter for use in radar, together with precision timing methods, opened the way to laboratory-based measurements of the speed of light. In 1946, Louis Essen and A.C. Gordon-Smith used a microwave cavity of precisely known dimensions to establish the frequency for a variety of normal modes of microwaves. As the wavelength of the modes was known from the geometry of the cavity and from electromagnetic theory, knowledge of the associated frequencies enabled a calculation of the speed of light.

The Essen-Gordon-Smith result, 299792±3 km/s, was substantially more precise than those found by optical techniques, and prompted much controversy. However, by 1950 repeated measurements by Essen established a result of 299792.5±1 km/s, which became the value adopted by the 12th General Assembly of the Radio-Scientific Union in 1957.

An idealized interferometric determination of wavelength obtained by looking at interference fringes between two coherent beams recombined after traveling different distances. Top: Constructive interference (in phase); If the difference in path length is a multiple of a wavelength, the recombined beams support one another and reconstitute the original beam. Bottom: Destructive interference (out of phase); If the two paths differ by half a wavelength, the recombined beams are out of phase and cancel each other. The bottom panel in the figure suggests the path length has been increased by half a wavelength by moving the right-hand point of reflection further out.

An alternative to the cavity resonator method to find the wavelength for determining the speed of light is to use a form of interferometer, indicated schematically in the figure.[95] A coherent light beam with a known frequency, as from a laser, is split to follow two paths and then recombined. By carefully changing the path length and observing the interference pattern, the wavelength of the light can be determined, which can be related to the speed of light.

With modern electronics, particularly oscilloscopes with time resolutions of less than one nanosecond, the speed of light can now be directly measured by timing the delay of a light pulse from a laser or a LED in reflecting from a mirror, although this method is less precise than either the cavity resonator or the interferometric methods.[96][97][98]

Speed of light set by definition

See also: Metre

A change in the meaning of the term speed of light as used in the SI system of units occurred in 1983. In 1983 the 17th Conférence Générale des Poids et Mesures defined the metre to be the length of the path travelled by light in vacuum during a time interval of 1⁄299792458 of a second.[99] The reasons for using this definition are stated in Resolution 1.[100]

The effect of this definition is to redefine the term speed of light in vacuum as a conversion factor[101] with the exact value 299,792,458 m/s. The value of 299,792,458 m/s is approximately the measured value of the speed of light based upon the pre-1983 definition of the metre, and was selected in part to result in minimal dislocation of standards.[102] According to NIST:[103] “In all of these changes in definition, the goal was not only to improve the precision of the definition, but also to change its actual length as little as possible.” Thus, within the SI system of units, the speed of light is now a defined constant[9] and no longer something to be measured.[104] Improved experimental techniques do not affect the conversion factor speed of light, but do result in a better realization of the metre.[105] Because the second is defined in terms of atomic transitions that can be measured accurately, the new definition, being a ratio of measured times, allows for a definition of the metre with greater accuracy in practical measurement than one based on a ratio of lengths determined using a fringe count of interference patterns.[7]

Rather than measure a time-of-flight, one implementation of this definition is to use a recommended source with established frequency f, and delineate the metre in terms of the wavelength λ of this light as determined using the defined numerical value of c and the relationship λ = c / f.[106] Practical realizations of the metre use recommended wavelengths of visible light in a laboratory vacuum with corrections being applied to take account of actual conditions such as diffraction, gravitation or imperfection in the vacuum.

The term ‘vacuum’ is used in this definition and in this article to refer to the reference state of free space. Like absolute zero, it is an idealized state that only can be approximated in the physical world. Measurements in any real-world medium, such as air[107][108] or a medium perturbed by gravity must be corrected so as to relate to ‘vacuum’.

Physical quantities and their units

It is important to separate the definition of a physical quantity itself from the definition of the unit in which it is measured.[109] Measurement is basically comparison between the quantity being measured and the standard unit; it is a matter of ratios.[110] Setting the speed of light to a definite numerical value when measured in the SI units of m/s simply means comparisons of length are equivalent to comparisons of transit times of light.[7][111]

See also

References

Footnotes

  1. ^ Uzan, J-P; Leclercq, B (2008). The Natural Laws of the Universe: Understanding Fundamental Constants. Springer. pp. 43–44. ISBN 0387734546.
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  5. ^ Schwinger, JS (2002) [1986]. "Gravitational waves". Einstein's Legacy: The Unity of Space and Time (Reprint ed.). Courier Dover. p. 223. ISBN 0486419746. {{cite book}}: External link in |chapterurl= (help); Unknown parameter |chapterurl= ignored (|chapter-url= suggested) (help)
  6. ^ Wei-Tou Ni (2005). "Empirical foundation of the relativistic gravity" (PDF). Intl J Modern Physics D. 14: 901–921.
  7. ^ a b c Sydenham, PH (2003). "Measurement of length". In Walt Boyes (ed.). Instrumentation Reference Book (3rd ed.). Butterworth-Heinemann. p. 56. ISBN 0750671238. ... if the speed of light is defined as a fixed number then, in principle, the time standard will serve as the length standard ... {{cite book}}: External link in |chapterurl= (help); Unknown parameter |chapterurl= ignored (|chapter-url= suggested) (help) Cite error: The named reference "Boyes" was defined multiple times with different content (see the help page).
  8. ^ "Fundamental Physical Constants: Speed of Light in Vacuum". NIST. Retrieved 2009-08-21.
  9. ^ a b Jespersen, J; Fitz-Randolph, J; Robb, J (1999). From Sundials to Atomic Clocks: Understanding time and frequency (Reprint of National Bureau of Standards 1977, 2nd ed.). Courier Dover. p. 280. ISBN 0486409139.
  10. ^ Gibbs, P (1997). "Why Is c the Symbol For the Speed of Light?". University of California, Riverside. Retrieved 2008-08-20.
  11. ^ See for example:
  12. ^ The International System of Units (PDF) (9th ed.), International Bureau of Weights and Measures, Dec 2022, p. 112, ISBN 978-92-822-2272-0
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  31. ^ One such paradox is called the tachyonic antitelephone. See Tolman, RC (1917). The Theory of the Relativity of Motion. p. 54.
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  93. ^ a b c Teuber, J (2004). "Ole Rømer og den bevaegede Jord – en dansk førsteplads?". In Friedrichsen, P; Henningsen, O; Olsen, O; Thykier, C; Tortzen, CG (ed.). Ole Rømer – videnskabsmand og samfundstjener. Kroppedal, Studier i astronomi, Nyere tid, Arkaeologi. Gads Forlag. pp. 217–219.{{cite book}}: CS1 maint: multiple names: editors list (link) Template:Da icon
  94. ^ The history of these events has often been incorrectly reported, and the reader might wonder if it is correctly reported here. An account of this historical mix-up is found in French, AP (1990). "Roemer: a cautionary tale". In Roche, J (ed.). Physicists look back: studies in the history of physics. CRC Press. pp. 120–121. ISBN 0852740018.
  95. ^ A detailed discussion of the interferometer and its use for determining the speed of light can be found in Vaughan, JM (1989). The Fabry-Perot interferometer. CRC Press. p. 47 & pp. 384–391. ISBN 0852741383.
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  99. ^ "Base unit definitions: Meter". NIST. Retrieved 2009-08-22.
  100. ^ "Resolution 1". Conférence Générale des Poids et Mesures. BIPM. 1983. Retrieved 2009-08-23.
  101. ^ Jespersen, J; Fitz-Randolph, J; Robb, J (1999). From Sundials to Atomic Clocks: Understanding time and frequency (Reprint of National Bureau of Standards 1977, 2nd ed.). Courier Dover. p. 280. ISBN 0486409139. One fallout of the new defintion was that the speed of light was no longer a measured quantity … defining one unit [length] in terms of another [time] removes a constant of nature by turning c into a conversion factor whose value is fixed and arbitrary.
  102. ^ Edwin F. Taylor, John Archibald Wheeler (1992). Spacetime physics: introduction to special relativity (2nd ed.). Macmillan. ISBN 0716723271.
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  104. ^ Sullivan, DB. "Speed of Light From Direct Frequency and Wavelength Measurements" (PDF). NIST. p. 191. Retrieved 2009-08-22. A consequence of this definition is that the speed of light is now a defined constant, not to be measured again.
  105. ^ Steve Adams (1997). Relativity: an introduction to space-time physics. CRC Press. p. 140. ISBN 0748406212. One peculiar consequence of this system of definitions is that any future refinement in our ability to measure c will not change the speed of light (which is a defined number), but will change the length of the meter!
  106. ^ A list of the resulting wavelengths based upon these frequencies and λ = c/f is found at BIPM mise-en-pratique, method b.
  107. ^ Zagar, BG (1999). "Laser Interferometer Displacement Sensors; §6.5". In JG Webster, JG (ed.). The Measurement, Instrumentation, and Sensors Handbook. CRC Press. p. 6-69. ISBN 0849383471. {{cite book}}: External link in |chapterurl= (help); Unknown parameter |chapterurl= ignored (|chapter-url= suggested) (help)
  108. ^ Flügge, J (2004). "Fundamental length metrology: Practical issues; §D.2.1.3". In Webb, CE; JDC Jones, JDC (ed.). Handbook of Laser Technology and Applications. Taylor & Francis. pp. 1737 ff. ISBN 0750309660. {{cite book}}: External link in |chapterurl= (help); Unknown parameter |chapterurl= ignored (|chapter-url= suggested) (help); Unknown parameter |coauthors= ignored (|author= suggested) (help)CS1 maint: multiple names: editors list (link)
  109. ^ Cardwell, DA; Ginley, DS (2003). Characterization, Applications and Cryogenics. CRC Press. p. 1251. ISBN 0750308974.
  110. ^ Smolin, L (2007). The Trouble with Physics: The Rise of String Theory, the Fall of a Science, and What Comes Next. Houghton Mifflin Harcourt. p. 215. ISBN 061891868X.
  111. ^ Z. Bay, G. G. Luther, and J. A. White (1972). "Measurement of an Optical Frequency and the Speed of Light". Phys. Rev. Lett. 29: 189–192. doi:10.1103/PhysRevLett.29.189.{{cite journal}}: CS1 maint: multiple names: authors list (link)

Historical references

Modern references

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