Shopping on line can be easy, simple and save you lots of money. It can also take a lot of your time, frustrate you, and result in unwanted purchases. Now the same can be said for regular high street shopping, but with the vast opportunity presented by the Internet it will pay you to spend a few minutes reading this and understanding how to better optimize your Speed Of Light shopping experience:
1. Compare - without doubt the biggest advantage that the Speed Of Light offers shoppers today is the ability to compare thousands of Speed Of Light at a time. This is a great thing, but not necessarily all the time! Too much can be daunting at times so take advantage of the great comparison sites and where possible let them do the hard work for you.
2. Research - if it has been said it will be on the internet. Ignorance is no longer a justifiable reason for buying the wrong thing. Take the time to research in detail everything that you could possible want to know about
3. Testimonials - don't know anybody that has bought a Speed Of Light? Wrong! If the Speed Of Light is good the internet will let you know. Use the Internet as a friend and get testimonials before you buy.
4. Questions - Got a question about Speed Of Light then search the Forums, FAQ's, Blogs etc. Don't be afraid to ask .....
5. Reputation - Never heard of the company selling Speed Of Light? Don't worry, no reason why you should know every company in the world, but you know someone that does! Use the internet to find out what people are saying about Speed Of Light and build up a picture of their reputation for sales, returns, customer service, delivery etc.
6. Returns - still worried that even after all of the above your Speed Of Light wont be what you want? Check out the returns policy. There is so much competition now that someone, somewhere is bound to offer the terms that you are comfortable with.
7. Feedback - happy with your Speed Of Light then let people know, after all you are depending on others people input in your buying decision, so why not give a little back.
8. Security - check for the yellow padlock on the Speed Of Light site before you buy, and the s after http:/ /i.e. https:// = a secure site
9. Contact - got a question about Speed Of Light, or want to leave a comment then check out the sites contact page. Reputable companies have them and respond.
10. Payment - ready to pay for your Speed Of Light, then use your credit card or PayPal! Be aware of companies that don't accept them, there may be genuine reasons but given the huge amount of choice you have when buying online there is no reason at all not to buy via credit card or PayPal.
"Lightspeed" redirects here. For other uses, see Lightspeed (disambiguation).
For the song "Speed of Light" see Episode (album)
The
speed of light in a vacuum is an important physical constant denoted by the letter
c for
constant or the Latin word
celeritas meaning "swiftness". It is the speed of all
electromagnetic radiation, including visible light, in a vacuum. More generally, it is the speed of anything having zero
rest mass.
and the Moon, about 1.2 seconds.
In metric units, the speed of light is exactly
Orders of magnitude (speed) metres per second (1,079,252,848.8 km/h). The fundamental
SI unit of length, the
metre, has been defined since
October 21, 1983, as the distance light travels in a vacuum in 1/299,792,458 of a
second; any increase in the precision of the measurement of the speed of light would refine the definition of the metre, but not alter the numerical value of
c. The approximate value of 3 m/s is commonly used in rough estimates. In imperial units, the speed of light is about 670,616,629.2 miles per hour or 983,571,056
feet per second, which is about 186,282.397 miles per second, or roughly one
Foot (unit of length) per nanosecond.
The speed of light when it passes through a transparency (optics) material medium, like glass or air, is slower than its speed in a vacuum. The ratio of
c to the observed
phase velocity is called the refractive index of the medium.
General relativity explains how a gravitational potential can affect the apparent speed of distant light in a vacuum, but locally light in a vacuum always passes an observer at a rate of
c.
Overview
One consequence of the laws of electromagnetism (such as Maxwell's equations) is that the speed
c of electromagnetic radiation does not depend on the velocity of the object emitting the radiation; thus for instance the light emitted from a rapidly moving light source would travel at the same speed as the light coming from a stationary light source (although the colour, frequency, energy, and momentum of the light will be shifted, which is called the
relativistic Doppler effect). If one combines this observation with the
principle of relativity, one concludes that all observers will measure the speed of light in vacuum as being the same, regardless of the
frame of reference of the observer or the velocity of the object emitting the light. Because of this fact, one can view
c as a fundamental physical constant. This logic is the basis of the theory of
special relativity.It is worth noting that it is the constant speed
c, rather than light itself, that is fundamental to special relativity; thus if light is somehow manipulated to travel at less than
c, this manipulation will not directly affect the theory of special relativity.
Observers traveling at large velocities will find that distances and times are distorted in accordance with the
Lorentz transformation; however, the transformations distort times and distances in such a way that the speed of light remains constant. A light sensor traveling near the speed of light would also find that colours of lights ahead were Blue shift and of those behind were redshifted, so that the Lorentz transformations and classical explanations of frequency shifting are in harmony.
If information could travel faster than
c in one reference frame, causality (physics) would be violated: in some other reference frames, the information would be received before it had been sent, so the 'effect' could be observed before the 'cause'. Due to special relativity's time dilation, the ratio between an external observer's perceived time and the time perceived by an observer moving closer and closer to the speed of light approaches zero. If something could move faster than light, this ratio would not be a real number. Such a violation of causality has never been recorded.
defines locations that are in
causality (physics) and those that are not.
To put it another way, information propagates to and from a point from 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').
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). However, there are also frames in which A precedes C (as shown) or in which C precedes A. Barring some way of traveling
faster than light, it is not possible for any matter (or information) to travel from A to C or from C to A. Thus there is no causal connection between A and C.
According to the currently prevailing definition, adopted in 1983, the speed of light is exactly 299,792,458 metres per second (approximately 3 metres per second, or about thirty centimetres (one foot (unit of length)) per
nanosecond). The value of c defines theVacuum permittivity (\epsilon_0) in SI units as:
\varepsilon_0 = 10^{7}/4\pi c^2 \quad \mathrm{(in~ A^2\, s^4\, kg^{-1}\, m^{-3}, \, or \, F \, m^{-1})}
The
magnetic constant \mu_0 is not dependent on c and is defined in SI units as:
\mu_0 = 4\,\pi\, 10^{-7} \quad \mathrm{(in~ kg\, m\, s^{-2}\, A^{-2}, \, or \, N \, A^{-2})}.
These constants appear in Maxwell's equations, which describe electromagnetism, and are related by:
c= \frac {1} {\sqrt{\varepsilon_0\mu_0-->
astronomy distances are sometimes measured in light years (the distance that light would travel in one year, roughly
1 E15 m kilometres or about 5.88 miles). Because light travels at a large but finite speed, it takes time for light to cover large distances. Thus, the light we observe from distant objects in the universe was emitted from them long ago: in effect, we see their distant past.
Communications and GPS
The speed of light is of relevance to
communications. For example, given the equatorial circumference of the
Earth is km and
c = km/s, the theoretical shortest amount of time for a piece of information to travel half the globe along the surface is s.
The actual transit time is longer, in part because the speed of light is slower by about 30% in an optical fiber and straight lines rarely occur in global communications situations, but also because delays are created when the signal passes through an electronic switch or signal regenerator. A typical time as of
2004 for a United States to Australia or Japan computer-to-computer
ping is 0.18 s. The speed of light additionally affects
wireless communications design.
Another consequence of the finite speed of light is that communications with spacecraft are not instantaneous, and the gap becomes more noticeable as distances increase. This delay was significant for communications between
Houston ground control and
Apollo 8 when it became the first spacecraft to orbit the Moon: For every question, Houston had to wait nearly 3 seconds for the answer to arrive, even when the astronauts replied immediately.
This effect forms the basis of the Global Positioning System (GPS), and similar navigation systems. One's position can be determined by means of the delays in radio signals received from a number of satellites, each carrying a very accurate
atomic clock, and very carefully synchronized. It is remarkable that, to work properly, this method requires that (among many other effects) the relative motion of satellite and receiver be taken into effect, which was how (on an interplanetary scale) the finite speed of light was originally discovered (see the following section).
Similarly, instantaneous remote control of interplanetary spacecraft is impossible because it takes time for the Earth-based controllers to receive information from the craft, and an equal time for instructions to be received by the craft. It can take hours for controllers to become aware of a problem, respond with instructions, and have the spacecraft receive the instructions.
The speed of light can also be of concern on very short distances. In
supercomputers, the speed of light imposes a limit on how quickly data can be sent between central processing units. If a processor operates at 1
GHz, a signal can only travel a maximum of 300 mm in a single cycle. Processors must therefore be placed close to each other to minimize communication latencies. If clock frequencies continue to increase, the speed of light will eventually become a limiting factor for the internal design of single
integrated circuit.
Physics
Constant velocity from all inertial reference frames
Most individuals are accustomed to the addition rule of velocities: if two cars approach each other from opposite directions, each traveling at a speed of 50 kilometres per hour, relative to the road surface, one expects that each car will perceive the other as approaching at a combined speed of 50 + 50 = 100 km/h to a very high degree of accuracy.
However, at velocities at or approaching the speed of light, this rule does not apply. Two spaceships approaching each other, each traveling at 90% the speed of light relative to some third observer between them, do not perceive each other as approaching at 90% + 90% = 180% the speed of light; instead they each perceive the other as approaching at slightly less than 99.5% the speed of light. This last result is given by the
Albert Einstein velocity addition formula:
u = {v + w \over 1 + v w / c^2} \,\!
where v and w are the (positive) speeds of the spaceships as observed by the third observer, and u is the speed of either space ship as observed by the other.Francis Weston Sears,
Introduction to the Theory of Relativity, p. 24, footnote: Except in giving a name to equation, the term "velocity" is used in this book to mean the speed and direction of motion. Velocity is a vector quantity, whereas speed refers only to the magnitude of the velocity. Since we have restricted motion to a single dimension (along the x-axis), we have not needed to introduce the concept of velocity here. This reduces to u = v + w for sufficiently small values of v and w (such as those typically encountered in common daily experiences), as the term v w / c^2 approaches zero, reducing the denominator to 1.
If one of the velocities for the above formula (or both) are
c, the final result is
c, as is expected if the speed of light is the same in all reference frames. Another important result comes from this formula always returning a value which is less than
c whenever
v and
w are less than
c: This shows that no acceleration in any frame of reference can cause you to exceed the speed of light with respect to another observer. Thus
c acts as a speed limit for all objects with respect to all other objects in special relativity.
Luminiferous aether (discredited)
Before the advent of special relativity, it was believed that light travels through a medium called the luminiferous aether. Maxwell’s equations predict a given speed of light, in much the same way as is the speed of
sound in
air. The speed of sound in air is relative to the movement of the air itself, and the speed of sound in air with respect to an observer may be changed if the observer is moving with respect to the air (or
wind). The speed of light was believed to be relative to a medium of transmission for light that acted as air does for the transmission of sound—the luminiferous aether.
The Michelson-Morley experiment, arguably the most famous and useful failed experiment in the history of physics, was designed to detect the motion of the Earth through the luminiferous aether. It could not find any trace of this kind of motion, suggesting, as a result, that it is impossible to detect one's presumed absolute motion, that is, motion with respect to the hypothesized luminiferous aether. The Michelson–Morley experiment said little about the speed of light relative to the light’s source and observer’s velocity, as both the source and observer in this experiment were traveling at the same velocity together in space.
Interaction with transparent materials
of a material indicates how much slower the speed of light is in that medium than in a vacuum. The slower speed of light in materials can cause refraction, as demonstrated by this triangular prism (optics) (in the case of a prism splitting white light into a
visible spectrum of colours, the refraction is known as
dispersion (optics)).
In passing through materials, the observed speed of light can differ from
c. The ratio of
c to the phase velocity of light in the material is called the refractive index. This apparent contradiction to the universality of the constant
c is a consequence of sloppy (but universally practiced) nomenclature: what is referred to as light in a medium is really a light-like hybrid of electromagnetic waves and mechanical oscillations of charged or magnetic particles such as
electrons or
ions, whereas light in the strict sense is a pure
electromagnetic wave (see further discussion below). The speed of light in Earth's atmosphere is only slightly less than c. Denser media, such as water and
glass, can slow light much more, to fractions such as ¾ and ⅔ of
c. Through diamond, light is much slower—only about 124,000 kilometres per second, less than ½ of
c. This reduction in speed is also responsible for bending of light at an interface between two materials with different indices, a phenomenon known as
refraction.
Since the speed of light in a material depends on the refractive index, and the refractive index depends on the frequency of the light, light at different frequencies travels at different speeds through the same material. This can cause distortion of electromagnetic waves that consist of multiple frequencies, an effect called
dispersion.
Note that the speed of light referred to is the observed or measured speed in some medium and not the true speed of light (as observed in vacuum). It may be noted, that once the light has emerged from the medium it changes back to its original speed and this is without gaining any energy. This can mean only one thing—that the light's speed itself was never altered in the first place.
It is sometimes claimed that light is slowed on its passage through a block of media by being absorbed and re-emitted by the atoms, only traveling at full speed through the vacuum between atoms. This explanation is incorrect and runs into problems if you try to use it to explain the details of refraction beyond the simple slowing of the signal.
Classically, considering electromagnetic radiation to be like a wave, the charges of each atom (primarily the electrons) interference with the electric and magnetic fields of the radiation, slowing its progress.
The full quantum-mechanical explanation is essentially the same, but has to cope with the discrete particle nature (see
Photon#Photons in matter): The E-field creates phonons in the media, and the
photons mix with the phonons. The resulting mixture, called a polariton, travels with a speed different from light.
Accelerated frames of reference and general relativity
Although it is constant in inertial frames of reference in special relativity, the speed of light can vary based on its position for accelerated frames of reference in special relativity and in general relativity. Before heading into this discussion, it must first be noted that in all cases the speed of light locally remains
c in these cases. So when an observer measures the speed of light at his own position, the constancy of its speed holds. The issue arises at positions distant from the observer in these situations.
The cause of this change is gravitational time dilation. As clocks at lower gravitational potentials tick slower, a beam of light will take longer to move along a rod at a lower gravitational potential than it would take to move along an identical rod at ones own potential. This light is considered to be moving more slowly at lower potentials. This slowdown becomes extreme as the light approaches the event horizon of a black hole, where both time and light will appear to stop. Similarly, light will appear to go faster at higher gravitational potentials.
In general relativity, the curvature of spacetime can also affect the number of rods between certain positions. This will add another factor to magnitude of the apparent speed change.
"Faster-than-light" observations and experiments
is Cherenkov radiation, emitted as a result of electrons traveling faster than the speed of light in water.
It has long been known theoretically that it is possible for the "group velocity" of light to exceed
c.
References
One recent experiment made the group velocity of laser beams travel for extremely short distances through caesium atoms at 300 times c
. In 2002, at the Université de Moncton, physicist Alain Haché made history by sending pulses at a group velocity of three times light speed over a long distance for the first time, transmitted through a 120-metre cable made from a coaxial photonic crystal. Electrical pulses break light speed record, physicsweb, 22 January 2002; see also A Haché and L Poirier (2002), Appl. Phys. Lett. v.80 p.518.However, it is not possible to use this technique to transfer information faster than c
: the velocity of information transfer depends on the front velocity (the speed at which the first rise of a pulse above zero moves forward) and the product of the group velocity and the front velocity is equal to the square of the normal speed of light in the material.Exceeding the group velocity of light in this manner is comparable to exceeding the speed of sound by arranging people distantly spaced in a line, and asking them all to shout "I'm here!", one after another with short intervals, each one timing it by looking at their own wristwatch so they don't have to wait until they hear the previous person shouting. Another example can be seen when watching ocean waves washing up on shore. With a narrow enough angle between the wave and the shoreline, the breakers travel along the waves' length much faster than the waves' movement inland.
The speed of light may also appear to be exceeded in some phenomena involving evanescent waves, such as quantum tunnelling. Experiments indicate that the
phase velocity and the group velocity of evanescent waves may exceed
c; however, it would appear that the front velocity does not exceed
c, so, again, it is not possible for information to be transmitted faster than
c.
In
quantum mechanics, certain quantum effects may be transmitted at speeds greater than
c (indeed,
action at a distance (physics) has long been perceived by some as a problem with quantum mechanics: see EPR paradox,
interpretations of quantum mechanics). For example, the
quantum states of two particles can be quantum entanglement, so the state of one particle fixes the state of the other particle (say, one must have
spin (physics) +½ and the other must have spin −½). Until the particles are observed, they exist in a
quantum superposition of two quantum states, (+½, −½) and (−½, +½). 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. If, as in some interpretations of quantum mechanics, one presumes that the information about the quantum state is local to one particle, then one must conclude that second particle takes up its quantum state instantaneously, as soon as the first observation is carried out. 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. The laws of physics also appear to prevent information from being transferred through more clever ways and this has led to the formulation of rules such as the no-cloning theorem and the
no-communication theorem.
So-called
superluminal motion is also seen in certain astronomical objects, such as the
relativistic jets of
radio galaxy 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.
Although it may sound paradoxical, it is possible for
shock waves to be formed with electromagnetic radiation. As a charged particle travels through an Electrical insulation medium, it disrupts the local electromagnetic field in the medium. Electrons in the atoms of the medium will be displaced and
polarization by the passing field of the charged particle, and photons are emitted as the electrons in the medium restore themselves to equilibrium after the disruption has passed. (In a
conductor (material), the equilibrium can be restored without emitting a photon.) In normal circumstances, these photons destructively interfere with each other and no radiation is detected. However, if the disruption travels faster than the photons themselves travel, as when a charged particle exceeds the speed of light in that medium, the photons constructively interfere and intensify the observed radiation. The result (analogous to a
sonic boom) is known as Cherenkov radiation.
The ability to communicate or travel faster-than-light is a popular topic in
science fiction. Particles that travel faster than light, dubbed tachyons, have been proposed by
particle physics but have yet to be observed, and would potentially violate causality if they were.
Some physicists, notably
João Magueijo and John Moffat, have proposed that in the past light traveled much faster than the current speed of light. This theory is called variable speed of light (VSL) and its supporters claim that it has the ability to explain many physical cosmology puzzles better than its rival, the
Cosmic inflation model of the universe. However, it has not gained wide acceptance.
"Slow light" experiments
phenomena, such as this rainbow, are due to the slower speed of light in a medium (water, in this case).
Light traveling through a medium other than a vacuum travels below c as a result of the time lag between the Polarization density response of the medium and the incident light. However, certain materials have an exceptionally high group index and a correspondingly low group velocity. In
1999, a team of scientists led by Lene Hau were able to slow the speed of a light pulse to about 17 metres per second; in 2001, they were able to momentarily stop a beam.
In
2003,
Mikhail Lukin, with 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.
History
Until relatively recent times, the speed of light was largely a matter of conjecture.
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". Furthermore, if light had a finite speed, it would have to be very great; Aristotle asserted "the strain upon our powers of belief is too great" to believe this.
One of the ancient theories of vision was that light was emitted from the eye, instead of entering the eye from another source. Using this 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.
Ancient, medieval and early modern theories
The 14th century Indian scholar
Sayana wrote in a comment on verse
RV 1.50.4 (1700–1100 BCE—the early Vedic period): "Thus it is remembered: Sun you who traverse 2202
yojanas 14,000 to 30,000 km in half a
nimesa 0.1 to 0.2 s", corresponding to between 65,000 and 300,000 km/s, for high values of
yojana and low values of
nimesa consistent with the
actual speed of light.{{cite web] initially agreed with
Aristotle's view that light has an infinite speed. In the
11th century, however,
Islamic science realized that light has a finite speed. The Iraqi Arab scientist
Ibn al-Haytham (Alhacen), the father of
optics, using an early
experimental scientific method in his
Book of Optics, discovered that light has a finite speed. Some of his contemporaries, notably the
Persian people scientists Avicenna and Abū Rayhān al-Bīrūnī, also agreed with Alhacen that light has a finite speed. Avicenna "observed that if the perception of light is due to the emission of some sort of particles by a luminous source, the speed of light must be finite."
George Sarton,
Introduction to the History of Science, Vol. 1, p. 710. Al-Biruni further discovered that the speed of light is much faster than the speed of sound.
Johannes Kepler believed that the speed of light is infinite since empty space presents no obstacle to it.
Francis Bacon (philosopher) argued that the speed of light is not necessarily infinite, since something can travel too fast to be perceived.
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 is infinite. Descartes was convinced that if the speed of light was finite, his whole system of philosophy would be demolished.
Measurement of the speed of light
Early attempts
Isaac Beeckman proposed an experiment (1629) in which a person would observe the flash of a
cannon reflecting off a
mirror about one mile away. Galileo Galilei proposed an experiment (1638), 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. This experiment was carried out by the Accademia del Cimento of
Florence in 1667, with the lanterns separated by about one mile. No delay was observed. 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. Descartes criticised this experiment as superfluous, in that the observation of eclipses, which had more power to detect a finite speed, gave a negative result.
Astronomical techniques
The first quantitative estimate of the speed of light was made in
1676 by Ole Rømer, who was studying the
motion (physics) of
Jupiter (planet) moon, Io (moon), with a telescope. It is possible to time the
orbital revolution of Io because it enters and exits Jupiter's shadow at regular interval (time)s (at C or D). 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. It was clear that these exit "signals" took longer to reach Earth, as Earth and Jupiter moved further apart. This was as a result of the extra time it took for light to cross the extra distance between the planets, time which had accumulated in the interval between one signal and the next. The opposite is the case when they are approaching (as from F to G). On the basis of his observations, Rømer estimated that it would take light 22 minutes to cross the diameter of the orbit of the Earth (that is, twice the
astronomical unit); the modern estimate is closer to 16 minutes and 40 seconds.
Around the same time, the astronomical unit was estimated to be about 140 million kilometres. The astronomical unit and Rømer's time estimate were combined by
Christiaan Huygens, who estimated the speed of light to be 1000 Earth diameters per minute. This is about 220,000 kilometres per second (136,000 miles per second), 26 per cent lower than the currently accepted value, but still very much faster than any physical phenomenon then known.
Isaac Newton also accepted the finite speed. In his 1704 book "Opticks" he reports the value of 16.6 Earth diameters per second (210,000 kilometres per second, 30% less than the actual value), which it seems he inferred for himself (whether from Rømer's data, or otherwise, is not known). The same effect was subsequently observed by Rømer for a "spot" rotating with the surface of Jupiter. And 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.
Even if, by these observations, the finite speed of light may not have been established to everyone's satisfaction (notably Giovanni Domenico Cassini's), after the observations of James Bradley (
1728), the hypothesis of infinite speed was considered discredited. 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 298,000 kilometres per second (185,000 miles per second). This is only slightly less than the currently accepted value. The aberration effect has been studied extensively over the succeeding centuries, notably by Friedrich Georg Wilhelm Struve and
Magnus Nyren.
.
Earth-bound techniques
The first successful measurement of the speed of light using an earthbound apparatus was carried out by Hippolyte Fizeau in
1849. (This measures the speed of light in air, which is slower than the speed of light in vacuum by a factor of the refractive index of air, about 1.0003.) Fizeau's experiment was conceptually similar to those proposed by Beeckman and Galileo. A beam of light was directed at a mirror several thousand metres 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 313,000 kilometres per second. Fizeau's method was later refined by
Marie Alfred Cornu (1872) and
Henri Joseph Anastase Perrotin (
1900).
Leon Foucault improved on Fizeau's method by replacing the cogwheel with a rotating mirror. Foucault's estimate, published in
1862, was 298,000 kilometres per second. Foucault's method was also used by Simon Newcomb and
Albert A. Michelson. Michelson began his lengthy career by replicating and improving on Foucault's method.
In 1926, Michelson used a rotating prism to measure the time it took light to make a round trip from
Mount Wilson (California) to
Mount San Antonio in
California. The precise measurements yielded a speed of 186,285 miles per second (299,796 kilometres per second).
Laboratory-based methods
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 in collaboration with A.C. Gordon-Smithused a microwave cavity of precisely known dimensions to establish the
frequency for a variety of
normal modes of microwaves—which, in common with all electromagnetic radiation, travels at the speed of light in vacuum. 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. Their result, 299,792±3 km/s, was substantially greater than those found by optical techniques, and prompted much controversy. However, by 1950 repeated measurements by
Essen established a result of 299,792.5±1 km/s; this became the value adopted by the 12th General Assembly of the
Radio-Scientific Union in
1957. Most subsequent measurements have been consistent with this value.
Speed of light set by definition
In 1983, the 17th Conférence Générale des Poids et Mesures adopted a standard value, 299,792,458 Metre per second for the speed of light. This in turn defines the length of a metre in terms of the speed of light, so that further refinements in the current experimental value of the speed of light would only refine the definition of a metre.
Relativity
From the work of James Clerk Maxwell, it was known that the speed of electromagnetic radiation was a constant defined by the electromagnetic properties of the vacuum (permittivity and permeability (electromagnetism)).
interferometer, as used for the Michelson-Morley experiment.
In
1887, the physicists
Albert Michelson and
Edward Morley performed the influential
Michelson-Morley experiment to measure the speed of light relative to the motion of the earth, the goal being to measure the velocity of the Earth through the "
luminiferous aether", the medium that was then thought to be necessary for the transmission of light. As shown in the diagram of a Michelson
interferometer, a
beam splitter was used to split a beam of monochromatic light into two beams traveling at
right angles to one another. After leaving the splitter, each beam was reflected back and forth between
mirrors several times (the same number for each beam to give a long but equal path length; the actual Michelson-Morley experiment used more
mirrors than shown) then recombined to produce a pattern of constructive and destructive interference. Any slight change in speed of light along each arm of the interferometer (because the apparatus was moving with the Earth through the proposed "aether") would change the amount of time that the beam spent in transit, which would then be observed as a change in the pattern of interference. In the event, the experiment gave a
null result.
Ernst Mach was among the first physicists to suggest that the experiment amounted to a disproof of the aether theory. Developments in theoretical physics had already begun to provide an alternative theory,
Lorentz-FitzGerald contraction hypothesis, which explained the null result of the experiment.
It is uncertain whether
Albert Einstein knew the results of the Michelson-Morley experiment, but the null result of the experiment greatly assisted the acceptance of his theory of relativity. The constant speed of light is one of the fundamental Postulates (together with causality (physics) and the
equivalence of inertial frames) of special relativity.
References
Footnotes
Historical references
- Ole Rømer. "Démonstration touchant le mouvement de la lumière", Journal des sçavans, 7 Décembre 1676, pp. 223–236. Translated as "A Demonstration concerning the Motion of Light", Philosophical Transactions of the Royal Society no. 136, pp. 893–894; June 25, 1677. (Rømer's 1676 paper, in English and French, as bitmap images, and in French as plain text)
- Edmund Halley. "Monsieur Cassini, his New and Exact Tables for the Eclipses of the First Satellite of Jupiter, reduced to the Julian Stile and Meridian of London", Philosophical Transactions XVIII, No. 214, pp 237–256, Nov.–Dec., 1694.
- H.L. Fizeau. "Sur une expérience relative à la vitesse de propogation de la lumière", Comptes Rendus 29, 90–92, 132, 1849.
- J.L. Foucault. "Détermination expérimentale de la vitesse de la lumière: parallaxe du Soleil", Comptes Rendus 55, 501–503, 792–796, 1862.
- A.A. Michelson. "Experimental Determination of the Velocity of Light", Proceedings of the American Association for the Advancement of Science 27, 71–77, 1878. ( Project Gutenberg Etext version)
- Simon Newcomb. "The Velocity of Light", Nature, pp 29–32, May 13, 1886.
- Joseph Perrotin. "Sur la vitesse de la lumière", Comptes Rendus 131, 731–734, 1900.
- A.A. Michelson, F.G. Pease, and F. Pearson. "Measurement Of The Velocity Of Light In A Partial Vacuum", Astrophysical Journal 82, 26–61, 1935.
Modern references
- Léon Brillouin. Wave propagation and group velocity. Academic Press Inc., 1960.
- John David Jackson. Classical electrodynamics. John Wiley & Sons, 2nd edition, 1975; 3rd edition, 1998. ISBN 0-471-30932-X
- R.J. MacKay and R.W. Oldford. "Scientific Method, Statistical Method and the Speed of Light", Statistical Science 15(3):254–278, 2000.
External links
- Speed of light in vacuum (at NIST)
- Definition of the metre (BIPM)
- Data Gallery: Michelson Speed of Light (Univariate Location Estimation) (download data gathered by Albert Abraham Michelson)
- Switching light on and off (news article on stopping light)
- Beam smashes light barrier (news article on group velocity experiment)
- Subluminal (Java applet demonstrating group velocity information limits)
- Light discussion on adding velocities
- Discussion on binary stars and adding of velocities
"Lightspeed" redirects here. For other uses, see Lightspeed (disambiguation).
For the song "Speed of Light" see Episode (album)
The
speed of light in a vacuum is an important physical constant denoted by the letter
c for
constant or the
Latin word
celeritas meaning "swiftness". It is the speed of all
electromagnetic radiation, including visible
light, in a
vacuum. More generally, it is the speed of anything having zero rest mass.
and the
Moon, about 1.2 seconds.
In metric units, the speed of light is exactly
Orders of magnitude (speed) metres per second (1,079,252,848.8 km/h). The fundamental SI unit of length, the metre, has been defined since October 21,
1983, as the distance light travels in a vacuum in 1/299,792,458 of a
second; any increase in the precision of the measurement of the speed of light would refine the definition of the metre, but not alter the numerical value of
c. The approximate value of 3 m/s is commonly used in rough estimates. In imperial units, the speed of light is about 670,616,629.2 miles per hour or 983,571,056 feet per second, which is about 186,282.397 miles per second, or roughly one
Foot (unit of length) per nanosecond.
The speed of light when it passes through a
transparency (optics) material medium, like glass or air, is slower than its speed in a vacuum. The ratio of
c to the observed
phase velocity is called the refractive index of the medium. General relativity explains how a
gravitational potential can affect the apparent speed of distant light in a vacuum, but locally light in a vacuum always passes an observer at a rate of
c.
Overview
One consequence of the laws of electromagnetism (such as Maxwell's equations) is that the speed
c of electromagnetic radiation does not depend on the velocity of the object emitting the radiation; thus for instance the light emitted from a rapidly moving light source would travel at the same speed as the light coming from a stationary light source (although the colour, frequency, energy, and momentum of the light will be shifted, which is called the relativistic Doppler effect). If one combines this observation with the principle of relativity, one concludes that all observers will measure the speed of light in vacuum as being the same, regardless of the
frame of reference of the observer or the velocity of the object emitting the light. Because of this fact, one can view
c as a fundamental physical constant. This logic is the basis of the theory of special relativity.It is worth noting that it is the constant speed
c, rather than light itself, that is fundamental to special relativity; thus if light is somehow manipulated to travel at less than
c, this manipulation will not directly affect the theory of special relativity.
Observers traveling at large velocities will find that distances and times are distorted in accordance with the
Lorentz transformation; however, the transformations distort times and distances in such a way that the speed of light remains constant. A light sensor traveling near the speed of light would also find that colours of lights ahead were
Blue shift and of those behind were redshifted, so that the Lorentz transformations and classical explanations of frequency shifting are in harmony.
If information could travel faster than
c in one reference frame,
causality (physics) would be violated: in some other reference frames, the information would be received before it had been sent, so the 'effect' could be observed before the 'cause'. Due to special relativity's time dilation, the ratio between an external observer's perceived time and the time perceived by an observer moving closer and closer to the speed of light approaches zero. If something could move faster than light, this ratio would not be a real number. Such a violation of causality has never been recorded.
defines locations that are in causality (physics) and those that are not.
To put it another way, information propagates to and from a point from 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').
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). However, there are also frames in which A precedes C (as shown) or in which C precedes A. Barring some way of traveling faster than light, it is not possible for any matter (or information) to travel from A to C or from C to A. Thus there is no causal connection between A and C.
According to the currently prevailing definition, adopted in 1983, the speed of light is exactly 299,792,458 metres per second (approximately 3 metres per second, or about thirty
centimetres (one
foot (unit of length)) per
nanosecond). The value of c defines theVacuum permittivity (\epsilon_0) in
SI units as:
\varepsilon_0 = 10^{7}/4\pi c^2 \quad \mathrm{(in~ A^2\, s^4\, kg^{-1}\, m^{-3}, \, or \, F \, m^{-1})}
The
magnetic constant \mu_0 is not dependent on c and is defined in SI units as:
\mu_0 = 4\,\pi\, 10^{-7} \quad \mathrm{(in~ kg\, m\, s^{-2}\, A^{-2}, \, or \, N \, A^{-2})}.
These constants appear in Maxwell's equations, which describe electromagnetism, and are related by:
c= \frac {1} {\sqrt{\varepsilon_0\mu_0-->
astronomy distances are sometimes measured in
light years (the distance that light would travel in one year, roughly 1 E15 m kilometres or about 5.88 miles). Because light travels at a large but finite speed, it takes time for light to cover large distances. Thus, the light we observe from distant objects in the universe was emitted from them long ago: in effect, we see their distant past.
Communications and GPS
The speed of light is of relevance to
communications. For example, given the equatorial circumference of the Earth is km and
c = km/s, the theoretical shortest amount of time for a piece of information to travel half the globe along the surface is s.
The actual transit time is longer, in part because the speed of light is slower by about 30% in an
optical fiber and straight lines rarely occur in global communications situations, but also because delays are created when the signal passes through an electronic switch or signal regenerator. A typical time as of 2004 for a United States to Australia or Japan computer-to-computer
ping is 0.18 s. The speed of light additionally affects wireless communications design.
Another consequence of the finite speed of light is that communications with spacecraft are not instantaneous, and the gap becomes more noticeable as distances increase. This delay was significant for communications between
Houston ground control and Apollo 8 when it became the first spacecraft to orbit the
Moon: For every question, Houston had to wait nearly 3 seconds for the answer to arrive, even when the astronauts replied immediately.
This effect forms the basis of the Global Positioning System (GPS), and similar
navigation systems. One's position can be determined by means of the delays in radio signals received from a number of satellites, each carrying a very accurate atomic clock, and very carefully
synchronized. It is remarkable that, to work properly, this method requires that (among many other effects) the relative motion of satellite and receiver be taken into effect, which was how (on an interplanetary scale) the finite speed of light was originally discovered (see the following section).
Similarly, instantaneous remote control of interplanetary spacecraft is impossible because it takes time for the Earth-based controllers to receive information from the craft, and an equal time for instructions to be received by the craft. It can take hours for controllers to become aware of a problem, respond with instructions, and have the spacecraft receive the instructions.
The speed of light can also be of concern on very short distances. In supercomputers, the speed of light imposes a limit on how quickly data can be sent between central processing units. If a processor operates at 1
GHz, a signal can only travel a maximum of 300 mm in a single cycle. Processors must therefore be placed close to each other to minimize communication latencies. If clock frequencies continue to increase, the speed of light will eventually become a limiting factor for the internal design of single
integrated circuit.
Physics
Constant velocity from all inertial reference frames
Most individuals are accustomed to the addition rule of velocities: if two cars approach each other from opposite directions, each traveling at a speed of 50 kilometres per hour, relative to the road surface, one expects that each car will perceive the other as approaching at a combined speed of 50 + 50 = 100 km/h to a very high degree of accuracy.
However, at velocities at or approaching the speed of light, this rule does not apply. Two spaceships approaching each other, each traveling at 90% the speed of light relative to some third observer between them, do not perceive each other as approaching at 90% + 90% = 180% the speed of light; instead they each perceive the other as approaching at slightly less than 99.5% the speed of light. This last result is given by the Albert Einstein
velocity addition formula:
u = {v + w \over 1 + v w / c^2} \,\!
where v and w are the (positive) speeds of the spaceships as observed by the third observer, and u is the speed of either space ship as observed by the other.Francis Weston Sears,
Introduction to the Theory of Relativity, p. 24, footnote: Except in giving a name to equation, the term "velocity" is used in this book to mean the speed and direction of motion. Velocity is a vector quantity, whereas speed refers only to the magnitude of the velocity. Since we have restricted motion to a single dimension (along the x-axis), we have not needed to introduce the concept of velocity here. This reduces to u = v + w for sufficiently small values of v and w (such as those typically encountered in common daily experiences), as the term v w / c^2 approaches zero, reducing the denominator to 1.
If one of the velocities for the above formula (or both) are
c, the final result is
c, as is expected if the speed of light is the same in all reference frames. Another important result comes from this formula always returning a value which is less than
c whenever
v and
w are less than
c: This shows that no acceleration in any frame of reference can cause you to exceed the speed of light with respect to another observer. Thus
c acts as a speed limit for all objects with respect to all other objects in special relativity.
Luminiferous aether (discredited)
Before the advent of special relativity, it was believed that light travels through a medium called the
luminiferous aether. Maxwell’s equations predict a given speed of light, in much the same way as is the speed of sound in
air. The speed of sound in air is relative to the movement of the air itself, and the speed of sound in air with respect to an observer may be changed if the observer is moving with respect to the air (or wind). The speed of light was believed to be relative to a medium of transmission for light that acted as air does for the transmission of sound—the luminiferous aether.
The Michelson-Morley experiment, arguably the most famous and useful failed experiment in the history of physics, was designed to detect the motion of the Earth through the luminiferous aether. It could not find any trace of this kind of motion, suggesting, as a result, that it is impossible to detect one's presumed absolute motion, that is, motion with respect to the hypothesized luminiferous aether. The Michelson–Morley experiment said little about the speed of light relative to the light’s source and observer’s velocity, as both the source and observer in this experiment were traveling at the same velocity together in space.
Interaction with transparent materials
of a material indicates how much slower the speed of light is in that medium than in a vacuum. The slower speed of light in materials can cause
refraction, as demonstrated by this triangular prism (optics) (in the case of a prism splitting white light into a visible spectrum of colours, the refraction is known as
dispersion (optics)).
In passing through materials, the observed speed of light can differ from
c. The ratio of
c to the phase velocity of light in the material is called the refractive index. This apparent contradiction to the universality of the constant
c is a consequence of sloppy (but universally practiced) nomenclature: what is referred to as light in a medium is really a light-like hybrid of electromagnetic waves and mechanical oscillations of charged or magnetic particles such as
electrons or ions, whereas light in the strict sense is a pure electromagnetic wave (see further discussion below). The speed of light in
Earth's atmosphere is only slightly less than c. Denser media, such as water and
glass, can slow light much more, to fractions such as ¾ and ⅔ of
c. Through diamond, light is much slower—only about 124,000 kilometres per second, less than ½ of
c. This reduction in speed is also responsible for bending of light at an interface between two materials with different indices, a phenomenon known as refraction.
Since the speed of light in a material depends on the refractive index, and the refractive index depends on the frequency of the light, light at different frequencies travels at different speeds through the same material. This can cause distortion of electromagnetic waves that consist of multiple frequencies, an effect called dispersion.
Note that the speed of light referred to is the observed or measured speed in some medium and not the true speed of light (as observed in vacuum). It may be noted, that once the light has emerged from the medium it changes back to its original speed and this is without gaining any energy. This can mean only one thing—that the light's speed itself was never altered in the first place.
It is sometimes claimed that light is slowed on its passage through a block of media by being absorbed and re-emitted by the atoms, only traveling at full speed through the vacuum between atoms. This explanation is incorrect and runs into problems if you try to use it to explain the details of refraction beyond the simple slowing of the signal.
Classically, considering electromagnetic radiation to be like a wave, the charges of each atom (primarily the
electrons)
interference with the electric and magnetic fields of the radiation, slowing its progress.
The full quantum-mechanical explanation is essentially the same, but has to cope with the discrete particle nature (see
Photon#Photons in matter): The E-field creates
phonons in the media, and the photons mix with the phonons. The resulting mixture, called a
polariton, travels with a speed different from light.
Accelerated frames of reference and general relativity
Although it is constant in inertial frames of reference in special relativity, the speed of light can vary based on its position for accelerated frames of reference in special relativity and in general relativity. Before heading into this discussion, it must first be noted that in all cases the speed of light locally remains
c in these cases. So when an observer measures the speed of light at his own position, the constancy of its speed holds. The issue arises at positions distant from the observer in these situations.
The cause of this change is gravitational time dilation. As clocks at lower gravitational potentials tick slower, a beam of light will take longer to move along a rod at a lower gravitational potential than it would take to move along an identical rod at ones own potential. This light is considered to be moving more slowly at lower potentials. This slowdown becomes extreme as the light approaches the event horizon of a black hole, where both time and light will appear to stop. Similarly, light will appear to go faster at higher gravitational potentials.
In general relativity, the curvature of spacetime can also affect the number of rods between certain positions. This will add another factor to magnitude of the apparent speed change.
"Faster-than-light" observations and experiments
is Cherenkov radiation, emitted as a result of electrons traveling faster than the speed of light in water.
It has long been known theoretically that it is possible for the "group velocity" of light to exceed
c.
References
One recent experiment made the group velocity of laser beams travel for extremely short distances through caesium atoms at 300 times c
. In 2002, at the Université de Moncton, physicist Alain Haché made history by sending pulses at a group velocity of three times light speed over a long distance for the first time, transmitted through a 120-metre cable made from a coaxial photonic crystal. Electrical pulses break light speed record, physicsweb, 22 January 2002; see also A Haché and L Poirier (2002), Appl. Phys. Lett. v.80 p.518.However, it is not possible to use this technique to transfer information faster than c
: the velocity of information transfer depends on the front velocity (the speed at which the first rise of a pulse above zero moves forward) and the product of the group velocity and the front velocity is equal to the square of the normal speed of light in the material.Exceeding the group velocity of light in this manner is comparable to exceeding the speed of sound by arranging people distantly spaced in a line, and asking them all to shout "I'm here!", one after another with short intervals, each one timing it by looking at their own wristwatch so they don't have to wait until they hear the previous person shouting. Another example can be seen when watching ocean waves washing up on shore. With a narrow enough angle between the wave and the shoreline, the breakers travel along the waves' length much faster than the waves' movement inland.
The speed of light may also appear to be exceeded in some phenomena involving
evanescent waves, such as quantum tunnelling. Experiments indicate that the phase velocity and the group velocity of evanescent waves may exceed
c; however, it would appear that the front velocity does not exceed
c, so, again, it is not possible for information to be transmitted faster than
c.
In quantum mechanics, certain quantum effects may be transmitted at speeds greater than
c (indeed,
action at a distance (physics) has long been perceived by some as a problem with quantum mechanics: see EPR paradox,
interpretations of quantum mechanics). For example, the quantum states of two particles can be
quantum entanglement, so the state of one particle fixes the state of the other particle (say, one must have
spin (physics) +½ and the other must have spin −½). Until the particles are observed, they exist in a
quantum superposition of two quantum states, (+½, −½) and (−½, +½). 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. If, as in some interpretations of quantum mechanics, one presumes that the information about the quantum state is local to one particle, then one must conclude that second particle takes up its quantum state instantaneously, as soon as the first observation is carried out. 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. The laws of physics also appear to prevent information from being transferred through more clever ways and this has led to the formulation of rules such as the
no-cloning theorem and the no-communication theorem.
So-called superluminal motion is also seen in certain astronomical objects, such as the relativistic jets of radio galaxy 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.
Although it may sound paradoxical, it is possible for
shock waves to be formed with electromagnetic radiation. As a charged particle travels through an
Electrical insulation medium, it disrupts the local electromagnetic field in the medium. Electrons in the atoms of the medium will be displaced and
polarization by the passing field of the charged particle, and photons are emitted as the electrons in the medium restore themselves to equilibrium after the disruption has passed. (In a
conductor (material), the equilibrium can be restored without emitting a photon.) In normal circumstances, these photons destructively interfere with each other and no radiation is detected. However, if the disruption travels faster than the photons themselves travel, as when a charged particle exceeds the speed of light in that medium, the photons constructively interfere and intensify the observed radiation. The result (analogous to a
sonic boom) is known as
Cherenkov radiation.
The ability to communicate or travel faster-than-light is a popular topic in science fiction. Particles that travel faster than light, dubbed tachyons, have been proposed by
particle physics but have yet to be observed, and would potentially violate
causality if they were.
Some physicists, notably João Magueijo and
John Moffat, have proposed that in the past light traveled much faster than the current speed of light. This theory is called
variable speed of light (VSL) and its supporters claim that it has the ability to explain many physical cosmology puzzles better than its rival, the Cosmic inflation model of the
universe. However, it has not gained wide acceptance.
"Slow light" experiments
phenomena, such as this
rainbow, are due to the slower speed of light in a medium (water, in this case).
Light traveling through a medium other than a vacuum travels below c as a result of the time lag between the
Polarization density response of the medium and the incident light. However, certain materials have an exceptionally high group index and a correspondingly low group velocity. In 1999, a team of scientists led by Lene Hau were able to slow the speed of a light pulse to about 17 metres per second; in
2001, they were able to momentarily stop a beam.
In
2003,
Mikhail Lukin, with 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.
History
Until relatively recent times, the speed of light was largely a matter of conjecture. 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". Furthermore, if light had a finite speed, it would have to be very great; Aristotle asserted "the strain upon our powers of belief is too great" to believe this.
One of the ancient theories of vision was that light was emitted from the eye, instead of entering the eye from another source. Using this 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.
Ancient, medieval and early modern theories
The 14th century
Indian scholar Sayana wrote in a comment on verse
RV 1.50.4 (1700–1100 BCE—the early Vedic period): "Thus it is remembered: Sun you who traverse 2202 yojanas 14,000 to 30,000 km in half a nimesa 0.1 to 0.2 s", corresponding to between 65,000 and 300,000 km/s, for high values of
yojana and low values of
nimesa consistent with the
actual speed of light.{{cite web] initially agreed with
Aristotle's view that light has an infinite speed. In the 11th century, however,
Islamic science realized that light has a finite speed. The
Iraqi Arab scientist Ibn al-Haytham (Alhacen), the father of
optics, using an early
experimental scientific method in his
Book of Optics, discovered that light has a finite speed. Some of his contemporaries, notably the
Persian people scientists
Avicenna and Abū Rayhān al-Bīrūnī, also agreed with Alhacen that light has a finite speed. Avicenna "observed that if the perception of light is due to the emission of some sort of particles by a luminous source, the speed of light must be finite."
George Sarton,
Introduction to the History of Science, Vol. 1, p. 710. Al-Biruni further discovered that the speed of light is much faster than the speed of sound.
Johannes Kepler believed that the speed of light is infinite since empty space presents no obstacle to it. Francis Bacon (philosopher) argued that the speed of light is not necessarily infinite, since something can travel too fast to be perceived.
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 is infinite. Descartes was convinced that if the speed of light was finite, his whole system of philosophy would be demolished.
Measurement of the speed of light
Early attempts
Isaac Beeckman proposed an experiment (
1629) in which a person would observe the flash of a
cannon reflecting off a
mirror about one mile away.
Galileo Galilei proposed an experiment (1638), 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. This experiment was carried out by the Accademia del Cimento of Florence in
1667, with the lanterns separated by about one mile. No delay was observed. 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. Descartes criticised this experiment as superfluous, in that the observation of eclipses, which had more power to detect a finite speed, gave a negative result.
Astronomical techniques
The first quantitative estimate of the speed of light was made in 1676 by
Ole Rømer, who was studying the motion (physics) of Jupiter (planet) moon,
Io (moon), with a telescope. It is possible to time the orbital revolution of Io because it enters and exits Jupiter's shadow at regular interval (time)s (at C or D). 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. It was clear that these exit "signals" took longer to reach Earth, as Earth and Jupiter moved further apart. This was as a result of the extra time it took for light to cross the extra distance between the planets, time which had accumulated in the interval between one signal and the next. The opposite is the case when they are approaching (as from F to G). On the basis of his observations, Rømer estimated that it would take light 22 minutes to cross the diameter of the orbit of the Earth (that is, twice the astronomical unit); the modern estimate is closer to 16 minutes and 40 seconds.
Around the same time, the astronomical unit was estimated to be about 140 million kilometres. The astronomical unit and Rømer's time estimate were combined by
Christiaan Huygens, who estimated the speed of light to be 1000 Earth diameters per minute. This is about 220,000 kilometres per second (136,000 miles per second), 26 per cent lower than the currently accepted value, but still very much faster than any physical phenomenon then known.
Isaac Newton also accepted the finite speed. In his 1704 book "Opticks" he reports the value of 16.6 Earth diameters per second (210,000 kilometres per second, 30% less than the actual value), which it seems he inferred for himself (whether from Rømer's data, or otherwise, is not known). The same effect was subsequently observed by Rømer for a "spot" rotating with the surface of Jupiter. And 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.
Even if, by these observations, the finite speed of light may not have been established to everyone's satisfaction (notably
Giovanni Domenico Cassini's), after the observations of
James Bradley (
1728), the hypothesis of infinite speed was considered discredited. 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 298,000 kilometres per second (185,000 miles per second). This is only slightly less than the currently accepted value. The aberration effect has been studied extensively over the succeeding centuries, notably by
Friedrich Georg Wilhelm Struve and Magnus Nyren.
.
Earth-bound techniques
The first successful measurement of the speed of light using an earthbound apparatus was carried out by Hippolyte Fizeau in 1849. (This measures the speed of light in air, which is slower than the speed of light in vacuum by a factor of the refractive index of air, about 1.0003.) Fizeau's experiment was conceptually similar to those proposed by Beeckman and Galileo. A beam of light was directed at a mirror several thousand metres 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 313,000 kilometres per second. Fizeau's method was later refined by Marie Alfred Cornu (1872) and Henri Joseph Anastase Perrotin (1900).
Leon Foucault improved on Fizeau's method by replacing the cogwheel with a rotating mirror. Foucault's estimate, published in 1862, was 298,000 kilometres per second. Foucault's method was also used by Simon Newcomb and
Albert A. Michelson. Michelson began his lengthy career by replicating and improving on Foucault's method.
In
1926, Michelson used a rotating prism to measure the time it took light to make a round trip from Mount Wilson (California) to Mount San Antonio in California. The precise measurements yielded a speed of 186,285 miles per second (299,796 kilometres per second).
Laboratory-based methods
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 in collaboration with A.C. Gordon-Smithused a
microwave cavity of precisely known dimensions to establish the
frequency for a variety of normal modes of microwaves—which, in common with all electromagnetic radiation, travels at the speed of light in vacuum. 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. Their result, 299,792±3 km/s, was substantially greater than those found by optical techniques, and prompted much controversy. However, by
1950 repeated measurements by Essen established a result of 299,792.5±1 km/s; this became the value adopted by the 12th General Assembly of the
Radio-Scientific Union in 1957. Most subsequent measurements have been consistent with this value.
Speed of light set by definition
In
1983, the 17th Conférence Générale des Poids et Mesures adopted a standard value, 299,792,458 Metre per second for the speed of light. This in turn defines the length of a metre in terms of the speed of light, so that further refinements in the current experimental value of the speed of light would only refine the definition of a metre.
Relativity
From the work of James Clerk Maxwell, it was known that the speed of electromagnetic radiation was a constant defined by the electromagnetic properties of the vacuum (permittivity and
permeability (electromagnetism)).
interferometer, as used for the Michelson-Morley experiment.
In
1887, the physicists Albert Michelson and
Edward Morley performed the influential
Michelson-Morley experiment to measure the speed of light relative to the motion of the earth, the goal being to measure the velocity of the
Earth through the "luminiferous aether", the medium that was then thought to be necessary for the transmission of light. As shown in the diagram of a Michelson
interferometer, a beam splitter was used to split a beam of
monochromatic light into two beams traveling at right angles to one another. After leaving the splitter, each beam was reflected back and forth between mirrors several times (the same number for each beam to give a long but equal path length; the actual Michelson-Morley experiment used more
mirrors than shown) then recombined to produce a pattern of constructive and destructive interference. Any slight change in speed of light along each arm of the interferometer (because the apparatus was moving with the Earth through the proposed "aether") would change the amount of time that the beam spent in transit, which would then be observed as a change in the pattern of interference. In the event, the experiment gave a
null result.
Ernst Mach was among the first physicists to suggest that the experiment amounted to a disproof of the aether theory. Developments in theoretical physics had already begun to provide an alternative theory, Lorentz-FitzGerald contraction hypothesis, which explained the null result of the experiment.
It is uncertain whether
Albert Einstein knew the results of the Michelson-Morley experiment, but the null result of the experiment greatly assisted the acceptance of his theory of relativity. The constant speed of light is one of the fundamental Postulates (together with causality (physics) and the
equivalence of inertial frames) of special relativity.
References
Footnotes
Historical references
- Ole Rømer. "Démonstration touchant le mouvement de la lumière", Journal des sçavans, 7 Décembre 1676, pp. 223–236. Translated as "A Demonstration concerning the Motion of Light", Philosophical Transactions of the Royal Society no. 136, pp. 893–894; June 25, 1677. (Rømer's 1676 paper, in English and French, as bitmap images, and in French as plain text)
- Edmund Halley. "Monsieur Cassini, his New and Exact Tables for the Eclipses of the First Satellite of Jupiter, reduced to the Julian Stile and Meridian of London", Philosophical Transactions XVIII, No. 214, pp 237–256, Nov.–Dec., 1694.
- H.L. Fizeau. "Sur une expérience relative à la vitesse de propogation de la lumière", Comptes Rendus 29, 90–92, 132, 1849.
- J.L. Foucault. "Détermination expérimentale de la vitesse de la lumière: parallaxe du Soleil", Comptes Rendus 55, 501–503, 792–796, 1862.
- A.A. Michelson. "Experimental Determination of the Velocity of Light", Proceedings of the American Association for the Advancement of Science 27, 71–77, 1878. ( Project Gutenberg Etext version)
- Simon Newcomb. "The Velocity of Light", Nature, pp 29–32, May 13, 1886.
- Joseph Perrotin. "Sur la vitesse de la lumière", Comptes Rendus 131, 731–734, 1900.
- A.A. Michelson, F.G. Pease, and F. Pearson. "Measurement Of The Velocity Of Light In A Partial Vacuum", Astrophysical Journal 82, 26–61, 1935.
Modern references
- Léon Brillouin. Wave propagation and group velocity. Academic Press Inc., 1960.
- John David Jackson. Classical electrodynamics. John Wiley & Sons, 2nd edition, 1975; 3rd edition, 1998. ISBN 0-471-30932-X
- R.J. MacKay and R.W. Oldford. "Scientific Method, Statistical Method and the Speed of Light", Statistical Science 15(3):254–278, 2000.
External links
- Speed of light in vacuum (at NIST)
- Definition of the metre (BIPM)
- Data Gallery: Michelson Speed of Light (Univariate Location Estimation) (download data gathered by Albert Abraham Michelson)
- Switching light on and off (news article on stopping light)
- Beam smashes light barrier (news article on group velocity experiment)
- Subluminal (Java applet demonstrating group velocity information limits)
- Light discussion on adding velocities
- Discussion on binary stars and adding of velocities
Speed of light - Wikipedia, the free encyclopedia
The speed of light in the vacuum of free space is an important physical constant usually denoted by the letter c. [1] It is the speed of all electromagnetic radiation, including ...
BBC - Radio 4 In Our Time - The Speed of Light
Melvyn Bragg and three guests investigate the history of ideas: The Speed of Light ... Melvyn Bragg and guest explore the history of ideas. Thursday 9.00-9.45am, repeated 9.30pm.
Speed of Light!
Speed of light is 12000 Lunar orbits/Earth day ... SPEED OF LIGHT 299,792.458 km/s is the speed of light in vacuum. However, according to Einstein's theory of General Relativity ...
Speed of Light
Speed of Light Kyla, do you remember how the wavelength of the electromagnetic wave became shorter when the charge was vibrating faster? Right, but the wave seemed to move ...
Speed of Light
The SPEED OF LIGHT is 299,792,458 metres per second ... Zyra's site //// CONCEPTS //// SCIENCE //// SITE INDEX. Also see TIME and the relationship between frequency and wavelength
Caterham R500 Superlight feature - Speed of light - 2008 - Features ...
The Caterham R500 will reel in that light at the end of the tunnel in a blur of insane acceleration. Tom Ford prepares to get warped ...
Euro boffins increase speed of light - vnunet.com
Breakthrough has applications in optical networking ... Euro boffins increase speed of light . Breakthrough has applications in optical networking
Speed of Light -- from Eric Weisstein's World of Physics
Defined as c\equiv 2.99792458\times 10^8{\rm\ m\ s}^{-1} =2.99792458\times 10^{10}{\rm\ cm\ s}^{-1}. Define \chi\equiv 2.99792458, then c=\chi\times 10^{8}{\rm\ m\ s}^{-1}.
Speed of light may have changed recently - 30 June 2004 - New ...
The controversial finding is based on re-analysis of old data that has long been used to argue for exactly the opposite
The Speed of Light
Michael Fowler UVa Physics Department. Index of Lectures and Overview of the Course Link to Previous Lecture. Early Ideas about Light Propagation . As we shall soon see, attempts ...