Difference between revisions of "Light" - New World Encyclopedia

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{{otheruses|info=light}}
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{{dablink|For other senses of this word, see [[light (disambiguation)]].}}
  
 
[[Image:PrismAndLight.jpg|thumb|300px|Prism splitting light]]
 
[[Image:PrismAndLight.jpg|thumb|300px|Prism splitting light]]
'''Light''' is [[electromagnetic radiation]] with a [[wavelength]] that is visible to the [[eye]] or, in a technical or scientific setting, electromagnetic radiation of any wavelength.  The three basic [[dimension]]s of light (and of all electromagnetic radiation) are:
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'''Light''' is [[electromagnetic radiation]] with a [[wavelength]] that is visible to the [[eye]] ('''visible light''') or, in a [[technical]] or [[scientific]] context, [[electromagnetic radiation]] of any [[wavelength]].  The three basic [[dimension]]s of light (i.e., all electromagnetic radiation) are:
* [[intensity]] (or brilliance or [[amplitude]], perceived by humans as the brightness of the light),
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* [[Intensity (physics)|Intensity]] (or [[amplitude]]), which is related to the human perception of [[brightness]] of the light,
* [[frequency]] (or [[wavelength]], perceived by humans as the [[color]] of the light), and
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* [[Frequency]] (or [[wavelength]]), perceived by humans as the [[color]] of the light, and
* [[polarization]] (or angle of vibration and not perceptible by humans under ordinary circumstances)
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* [[Polarization]] (or angle of vibration), which is not perceptible by humans under ordinary circumstances.
Due to [[wave-particle duality]], light simultaneously exhibits properties of both [[wave]]s and [[Particle physics|particles]]. The precise nature of light is one of the key questions of modern [[physics]].
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Due to the [[wave-particle duality]] of [[matter]], light simultaneously exhibits properties of both [[wave]]s and [[Particle physics|particles]]. The precise nature of light is one of the key questions of modern [[physics]].
 
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==Visible electromagnetic radiation==
== Visible electromagnetic radiation==
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{{main|Visible spectrum}}
Visible light is the portion of the [[electromagnetic spectrum]] between the [[frequency|frequencies]] of 380&nbsp;[[Hertz#SI_Multiples|THz]] (3.8&times;10<sup>14</sup>&nbsp;[[hertz]]) and 750&nbsp;[[Hertz#SI_Multiples|THz]] (7.5&times;10<sup>14</sup>&nbsp;[[hertz]]).  The speed (<math>c</math>), [[frequency]] (<math>f</math> or <math>\nu</math>), and wavelength (<math>\lambda</math>) of a wave obey the relation:
 
 
 
:<math> c = f~\lambda \,\!</math>
 
 
 
Because the [[speed of light]] in a vacuum is fixed, visible light can also be characterised by its [[wavelength]] of between 400&nbsp;[[nanometre]]s (abbreviated 'nm') and 800&nbsp;nm (in a [[vacuum]]).
 
 
 
Light excites the [[rod cell]]s and [[cone cell]]s in the [[retina]] of the [[human eye]], creating [[electric]]al nerve impulses that travel up the [[optic nerve]] to the [[brain]], producing [[vision]].
 
  
 
==Speed of light==
 
==Speed of light==
 
{{main|Speed of light}}
 
{{main|Speed of light}}
  
Although some people speak of the "velocity of light", the word ''[[velocity]]'' should be reserved for [[vector]] quantities, that is, those with both [[magnitude]] and [[direction]].  The speed of light is a [[scalar]] quantity, having only magnitude and no direction, and therefore ''speed'' is the correct term.
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The speed of light in a vacuum is exactly 299,792,458 metres per second (fixed by definition). Although some people speak of the "velocity of light", the word ''[[velocity]]'' is usually reserved for [[vector (spatial)|vector]] quantities, which have a direction.
  
The speed of light has been measured many times, by many physicists. The best early measurement is [[Ole Rømer]]'s (a Danish physicist), in [[1676]]. By observing the motions of [[Jupiter (planet)|Jupiter]] and one of its [[natural satellite|moon]]s, [[Io (moon)|Io]], with a [[telescope]], and noting discrepancies in the apparent period of Io's orbit, Rømer calculated a speed of 227,000&nbsp;[[kilometre]]s per [[second]] (approximately 141,050&nbsp;[[mile]]s per second).
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Some scholars have conjectured that the speed of light was first known in [[India]], based on a statement by [[Sayana]] (c. [[1315]]-[[1387]]). [[Max Muller]]'s translation of Sayana's commentary on the [[Rig Veda]] states: "Thus it is remembered: [O Sun] you who traverse 2202 yojanas in half a nimesa." This corresponds to a speed of about 302,073 km/s, which is close to the speed of light (299,792 km/s). This statement also occurs in [[Bhatta Bhaskara]]'s earlier commentary on the ''[[Taittiriya Brahmana]]''. There is still much debate on whether Sayana was estimating the speed of light or overestimating the speed of the [[Sun]], since he didn't make it clear which he was referring to, nor did he give any methods for his estimate. {{inote|S. Kak, 1998}}
  
The first successful measurement of the speed of light using an earthbound apparatus was carried out by [[Hippolyte Fizeau]] in [[1849]]. Fizeau directed a beam of light at a mirror several thousand metres away, and placed a rotating cog wheel in the path of the beam from the source to the mirror and back again.  At a certain rate of rotation, the beam could pass through one gap in the wheel on the way out and the next gap on the way back. Knowing the distance to the mirror, the number of teeth on the wheel, and the rate of rotation, Fizeau measured the speed of light as 313,000&nbsp;kilometres per second.
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The speed of light has been measured many times, by many physicists. The best early measurement in Europe is by [[Ole Rømer]], a Danish physicist, in [[1676]]. By observing the motions of [[Jupiter (planet)|Jupiter]] and one of its [[natural satellite|moon]]s, [[Io (moon)|Io]], with a [[telescope]], and noting discrepancies in the apparent period of Io's orbit, Rømer calculated that
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light takes about 18 minutes to traverse the diameter of Earth's orbit. Had he known the diameter of the orbit in kilometers (which he didn't) he would have deduced a speed of 227,000&nbsp;[[kilometre]]s per [[second]] (approximately 141,050&nbsp;[[mile]]s per second).
  
[[Léon Foucault]] used rotating mirrors to obtain a value of  298,000&nbsp;km/s (about 185,000&nbsp;miles/s) in [[1862]].  [[Albert A. Michelson]] conducted experiments on the speed of light from [[1877]] until his death in 1931.  He refined Foucault's results in [[1926]] using improved rotating [[mirror]]s to measure the [[time]] it took light to make a round trip from Mt. Wilson to Mt. San Antonio in [[California]].  The precise measurements yielded a speed of 186,285&nbsp;mile/s (299,796&nbsp;km/s [1,079,265,600 km/h]).  In daily use, the figures are rounded off to 300,000&nbsp;km/s and 186,000&nbsp;miles/s.
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The first successful measurement of the speed of light in Europe using an earthbound apparatus was carried out by [[Hippolyte Fizeau]] in [[1849]]. Fizeau directed a beam of light at a mirror several thousand metres away, and placed a rotating cog wheel in the path of the beam from the source to the mirror and back again.  At a certain rate of rotation, the beam could pass through one gap in the wheel on the way out and the next gap on the way back. Knowing the distance to the mirror, the number of teeth on the wheel, and the rate of rotation, Fizeau measured the speed of light as 313,000&nbsp;kilometres per second.
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[[Léon Foucault]] used rotating mirrors to obtain a value of  298,000&nbsp;km/s (about 185,000&nbsp;miles/s) in [[1862]].  [[Albert A. Michelson]] conducted experiments on the speed of light from [[1877]] until his death in 1931.  He refined Foucault's results in [[1926]] using improved rotating [[mirror]]s to measure the [[time]] it took light to make a round trip from Mt. Wilson to Mt. San Antonio in [[California]].  The precise measurements yielded a speed of 186,285&nbsp;mi/s (299,796&nbsp;km/s [1,079,265,600 km/h]).  In daily use, the figures are rounded off to 300,000&nbsp;km/s and 186,000&nbsp;miles/s.
  
 
==Refraction==
 
==Refraction==
 
{{main|Refraction}}
 
{{main|Refraction}}
  
All light propagates at a finite speed.  Even moving observers always measure the same value of ''c'', the speed of light in [[vacuum]], as ''c'' = 299,792,458&nbsp;[[metre]]s per [[second]] (186,282.397 [[mile]]s per second).  When light passes through a transparent substance, such as air, water or glass, its speed is reduced, and it undergoes refraction.  The reduction of the speed of light in a denser material can be indicated by the [[refractive index]], ''n'', which is defined as:
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All light propagates at a finite speed.  Even moving observers always measure the same value of ''c'', the speed of light in [[vacuum]], as ''c'' = 299,792,458 [[metre]]s per [[second]] (186,282.397 [[mile]]s per second).  When light passes through a transparent substance, such as air, water or glass, its speed is reduced, and it undergoes [[refraction]].  The reduction of the speed of light in a denser material can be indicated by the [[refractive index]], ''n'', which is defined as:
 
 
 
:<math> n = \frac{c}{v} \;\!</math>
 
:<math> n = \frac{c}{v} \;\!</math>
  
Thus, ''n''=1 in a vacuum and ''n''>1 in matter.
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Thus, ''n'' = 1 in a vacuum and ''n'' > 1 in matter.
  
When a beam of light enters a medium from vacuum or another medium, it keeps the same frequency and changes its wavelength. If the incident beam is not orthogonal to the edge between the media, the direction of the beam will change.  Refraction of light by [[lens (optics)|lens]]es is used to focus light in [[magnifying glass]]es, [[spectacles]] and [[contact lens]]es, [[microscope]]s and [[refracting telescope]]s.
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When a beam of light enters a medium from vacuum or another medium, it keeps the same frequency and changes its wavelength. If the incident beam is not [[orthogonality|orthogonal]] to the edge between the media, the direction of the beam will change.  Refraction of light by [[lens (optics)|lens]]es is used to focus light in [[magnifying glass]]es, [[spectacles]] and [[contact lens]]es, [[microscope]]s and [[refracting telescope]]s.
  
 
==Optics==
 
==Optics==
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The study of light and the interaction of light and [[matter]] is termed [[optics]]. The observation and study of [[optical phenomenon|optical phenomena]] such as [[rainbow]]s offers many clues as to the nature of light as well as much enjoyment.
 
The study of light and the interaction of light and [[matter]] is termed [[optics]]. The observation and study of [[optical phenomenon|optical phenomena]] such as [[rainbow]]s offers many clues as to the nature of light as well as much enjoyment.
  
==Color and wavelengths==
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==Colour and wavelength==
The different wavelengths are detected by the human eye and then interpreted by the [[brain]] as [[color]]s, ranging from [[red]] at the longest wavelengths of about 700 nm. (lowest frequencies) to [[violet (color)|violet]] at the shortest wavelengths of about 400 nm. (highest frequencies). The intervening frequencies are seen as [[Orange (colour)|orange]], [[yellow]], [[green]], [[cyan]], [[blue]], and, conventionally, [[indigo]].  
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{{main|Colour}}
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The different wavelengths are detected by the human eye and then interpreted by the [[brain]] as colours, ranging from [[red]] at the longest wavelengths of about 700 nm to [[violet (colour)|violet]] at the shortest wavelengths of about 400 nm. The intervening frequencies are seen as [[Orange (colour)|orange]], [[yellow]], [[green]], and [[blue]].  
  
 
<BR>
 
<BR>
 
[[Image:spectrum4websiteEval.png|center|]]
 
[[Image:spectrum4websiteEval.png|center|]]
 
<BR>
 
<BR>
The wavelengths of the electromagnetic spectrum immediately outside the range that the human eye is able to perceive are called ''[[ultraviolet]]'' (UV) at the short wavelength (high frequency) end and ''[[infrared]]'' (IR) at the long wavelength (low frequency) end. Although humans cannot see IR, they do perceive the [[near infrared|near IR]] (shorter wavelength, higher frequency, higher energy) as [[heat]] through receptors in the [[skin]]. [[Camera]]s that can detect IR and convert it to light are called, depending on their application, [[night-vision]] cameras or [[infrared camera]]s (not to be confused with an [[image intensifier]] that only amplifies available visible light).
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The wavelengths of the electromagnetic spectrum immediately outside the range that the human eye is able to perceive are called ''[[ultraviolet]]'' (UV) at the short wavelength (high frequency) end and ''[[infrared]]'' (IR) at the long wavelength (low frequency) end. Some animals, such as [[bee]]s, can see UV radiation while others, such as [[pit viper]] [[snake]]s, can see infrared light.
  
UV radiation is not directly perceived by humans at all except in a very delayed fashion, as overexposure of the skin to UV light can cause [[sunburn]], or [[skin cancer]], and underexposure can cause [[Seasonal affective disorder|depression]] due to [[vitamin D]] deficiency. However, because UV is a higher frequency radiation than visible light, it very easily can cause materials to [[fluorescence|fluoresce]] visible light.  
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UV radiation is not normally directly perceived by humans except in a very delayed fashion, as overexposure of the skin to UV light can cause [[sunburn]], or [[skin cancer]], and underexposure can cause [[vitamin D]] deficiency. However, because UV is a higher frequency radiation than visible light, it very easily can cause materials to [[fluorescence|fluoresce]] visible light.  
  
Some animals, such as [[bee]]s, can see UV radiation while others, such as pit viper [[snake]]s, can see IR using pits in their heads.
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[[Camera]]s that can detect [[infrared|IR]] and convert it to light are called, depending on their application, [[night-vision]] cameras or [[infrared camera]]s. These are different from [[image intensifier]] cameras, which only amplify available visible light.
  
== Measurement of light ==
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When intense radiation (of any frequency) is absorbed in the skin, it causes [[heat]]ing which can be felt. Since hot objects are strong sources of infrared radiation, IR radiation is commonly associated with this sensation. Any intense radiation that can be absorbed in the skin will have the same effect, however.
The following quantities and units are used to measure light.
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*[[brightness]] (or temperature)
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==Measurement of light==
*illuminance or illumination ([[SI]] unit: [[lux]])
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{{main|photometry}}
*luminous [[flux]] (SI unit: [[lumen (unit)|lumen]])
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The following quantities and units are used to measure the quantity or "[[brightness]]" of light.
*luminous intensity (SI unit: [[candela]])
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{{SI_light_units}}
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{{SI_radiometry_units}}
  
 
Light can also be characterised by:
 
Light can also be characterised by:
*[[brilliance]] (or [[amplitude]]),
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*[[amplitude]],
*[[color]] (or [[frequency]]), and  
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*[[color]], [[wavelength]], or [[frequency]], and  
 
*[[polarization]] (or angle of vibration).
 
*[[polarization]] (or angle of vibration).
  
===SI light units===
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==Light sources==
{{SI_light_units}}
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{{seealso|List of light sources}}
 
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[[Image:Light beams in smoke03.jpg|thumb|250px|Sunlight scattered by smoke]]
== Light sources ==
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There are [[List of light sources|many sources of light]]. The most common light sources are thermal: a body at a given [[temperature]] emits a characteristic spectrum of [[black body]] radiation.  Examples include [[sunlight]] (the radiation emitted by the [[chromosphere]] of the [[Sun]] at around 6,000&nbsp;[[kelvin|K]] peaks in the visible region of the electromagnetic spectrum), [[incandescent light bulb]]s (which emit only around 10% of their energy as visible light and the remainder as infrared), and glowing solid particles in [[fire|flames]]. The peak of the blackbody spectrum is in the infrared for relatively cool objects like human beings. As the temperature increases, the peak shifts to shorter wavelengths, producing first a red glow, then a white one, and finally a blue color as the peak moves out of the visible part of the spectrum and into the ultraviolet. These colors can be seen when metal is [[heat]]ed to "red hot" or "white hot". The blue color is most commonly seen in a [[natural gas|gas]] flame or a welder's torch.
[[Image:Light beams in smoke03.jpg|thumb|250px|Sunlight visible in smoke]]
 
There are many sources of light. A body at a given [[temperature]] will emit a characteristic spectrum of [[black body]] radiation.  Examples include [[sunlight]] (the radiation emitted by the [[chromosphere]] of the [[Sun]] at around 6,000&nbsp;[[kelvin|K]] peaks in the visible region of the electromagnetic spectrum), [[incandescent light bulb]]s (which are generally very inefficient, emitting only around 10% of their energy as light and the remainder as "heat", i.e. infrared) and glowing solid particles in flames (see [[fire]], [[red hot]], [[white hot]]).
 
  
Atoms emit and absorb light at characteristic energies. [[Emission line]]s can either be [[stimulated emission|stimulated]], such as visible [[laser]]s and microwave [[maser]] emission, [[light-emitting diode]]s, [[gas discharge]] lamps (such as [[neon lamp]]s and [[neon sign]]s, [[mercury-vapor lamp]]s, etc), and flames (light from the hot gas itself - so, for example, [[sodium]] in a gas flame emits characteristic yellow light) or [[spontaneous emission|spontaneous]].
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Atoms emit and absorb light at characteristic energies. This produces "[[emission line]]s" in the spectrum of each atom. Emission can be [[spontaneous emission|spontaneous]], as in [[light-emitting diode]]s, [[gas discharge]] lamps (such as [[neon lamp]]s and [[neon sign]]s, [[mercury-vapor lamp]]s, etc.), and flames (light from the hot gas itself&mdash;so, for example, [[sodium]] in a gas flame emits characteristic yellow light). Emission can also be [[stimulated emission|stimulated]], as in a [[laser]] or a microwave [[maser]].  
  
Acceleration of a free charged particle, such as an [[electron]], can produce visible radiation:  [[Cyclotron radiation]], [[Synchrotron radiation]], and [[Bremsstrahlung]] radiation.  Particles moving through a medium faster than the speed of light in that medium can produce visible [[Cherenkov radiation]].
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Acceleration of a free charged particle, such as an [[electron]], can produce visible radiation:  [[cyclotron radiation]], [[synchrotron radiation]], and [[bremsstrahlung]] radiation are all examples of this.  Particles moving through a medium faster than the speed of light in that medium can produce visible [[Cherenkov radiation]].
  
Certain chemicals produce visible radiation by [[chemoluminescence]].  In living things, this process is called [[bioluminescence]]: for example, [[firefly|fireflies]] produce light by this means, and boats moving through water can disturb glowing plankton.
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Certain chemicals produce visible radiation by [[chemoluminescence]].  In living things, this process is called [[bioluminescence]]. For example, [[firefly|fireflies]] produce light by this means, and boats moving through water can disturb plankton which produce a glowing wake.
  
Certain substances produce light when they are illuminated by more energetic radiation, a process known as [[fluorescence]].  This is used in [[strip light]]s.
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Certain substances produce light when they are illuminated by more energetic radiation, a process known as [[fluorescence]].  This is used in [[Fluorescent lamp|fluorescent light]]s. Some substances emit light slowly after excitation by more energetic radiation. This is known as [[phosphorescence]].
  
Particles striking certain chemicals can produce light by [[phosphorescence]], for example, [[cathodoluminescence]].  This mechanism is used in [[oscilloscope]]s and [[televisions]], and [[cathode ray tube]].
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Phosphorescent materials can also be excited by bombarding them with subatomic particles. [[Cathodoluminescence]] is one example of this.  This mechanism is used in [[cathode ray tube]] [[television]]s.
  
 
Certain other mechanisms can produce light:
 
Certain other mechanisms can produce light:
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**[[scintillator]]
 
**[[scintillator]]
 
*[[electroluminescence]]
 
*[[electroluminescence]]
*[[bioluminescence]]
 
 
*[[sonoluminescence]]
 
*[[sonoluminescence]]
 
*[[triboluminescence]]
 
*[[triboluminescence]]
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*particle-[[antiparticle]] annihilation
 
*particle-[[antiparticle]] annihilation
  
== Theories about light ==
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==Theories about light==
=== Early Greek ideas ===
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===Indian theories===
In [[55 BC]] [[Lucretius]], continuing the ideas of earlier [[atomism|atomists]], wrote that light and heat from the Sun were composed of minute particles.
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In [[ancient India]], the philosophical schools of [[Samkhya]] and [[Vaisheshika]], from around the [[6th century B.C.E.|6th]]&ndash;[[5th century BC]], developed theories on light. According to the Samkhya school, light is one of the five fundamental "subtle" elements (''tanmatra'') out of which emerge the gross elements. The [[atomism|atomicity]] of these elements is not specifically mentioned and it appears that they were actually taken to be continuous.
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On the other hand, the Vaisheshika school gives an [[atomic theory]] of the physical world on the non-atomic ground of [[ether]], space and time. (See [[Atomism#Indian atomism|Indian atomism]].) The basic [[atom]]s are those of earth (''prthivı''), water (''apas''), fire (''tejas''), and air (''vayu''), that should not be confused with the ordinary meaning of these terms. These atoms are taken to form binary molecules that combine further to form larger molecules. Motion is defined in terms of the movement of the physical atoms and it appears that it is taken to be non-instantaneous. Light rays are taken to be a stream of high velocity of ''tejas'' (fire) atoms. The particles of light can exhibit different characteristics depending on the speed and the arrangements of the ''tejas'' atoms.
  
[[Ptolemy]] also wrote about the refraction of light.
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Later in [[499|499 C.E.]], [[Aryabhata]], who proposed a [[heliocentric]] [[solar system]] of [[gravitation]] in his ''Aryabhatiya'', wrote that the planets and the [[Moon]] do not have their own light but reflect the light of the [[Sun]].
  
=== 10th century optical theory ===
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The Indian [[Buddhist]]s, such as [[Dignāga]] in the [[5th century]] and [[Dharmakirti]] in the [[7th century]], developed a type of [[atomism]] that is a philosophy about reality being composed of atomic entities that are momentary flashes of light or energy. They viewed light as being an atomic entity equivalent to energy, similar to the modern concept of [[photon]]s, though they also viewed all matter as being composed of these light/energy particles.
The scientist Abu Ali al-Hasan ibn al-Haytham (965-c.1040), also known as [[Alhazen]], developed a broad theory that explained vision, using [[geometry]] and [[anatomy]], which stated that each point on an illuminated area or object radiates light rays in every direction, but that only one ray from each point, which strikes the eye perpendicularly, can be seen. The other rays strike at different angles and are not seen.  He used the example of the [[pinhole camera]], which produces an inverted image, to support his argument.  Alhazen held light rays to be streams of minute particles that travelled at a finite speed.  He improved [[Ptolemy]]'s theory of the [[refraction]] of light. Alhazen's work did not become known in Europe until the late [[16th century]].
 
  
=== The 'plenum' ===
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===Greek and Hellenistic theories===
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In the fifth century B.C.E., [[Empedocles]] postulated that everything was composed of [[four elements]]; fire, air, earth and water. He believed that [[Aphrodite]] made the human eye out of the four elements and that she lit the fire in the eye which shone out from the eye making sight possible. If this were true, then one could see during the night just as well as during the day, so Empedocles postulated an interaction between rays from the eyes and rays from a source such as the sun.
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In about 300 B.C.E., [[Euclid]] wrote ''Optica'', in which he studied the properties of light. Euclid postulated that light travelled in straight lines and he described the laws of reflection and studied them mathematically. He questioned that sight is the result of a beam from the eye, for he asks how one sees the stars immediately, if one closes ones eyes, then opens them at night. Of course if the beam from the eye travels infinitely fast this is not a problem.
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In [[55 B.C.E.]], [[Lucretius]], a Roman who carried on the ideas of earlier Greek [[atomism|atomists]], wrote:
 +
 
 +
"''The light and heat of the sun; these are composed of minute atoms which, when they are shoved off, lose no time in shooting right across the interspace of air in the direction imparted by the shove.''" - ''On the nature of the Universe''
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 +
Despite being remarkably similar to how we think of light today, Lucretius's views were not generally accepted and light was still theorized as emanating from the eye.
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 +
[[Ptolemy]] (c. [[2nd century|2nd century CE]]) wrote about the [[refraction]] of light, and developed a theory of vision that objects are seen by rays of light emanating from the eyes.
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===Optical theory===
 +
The [[Persia]]n scientist [[Alhazen|Alhazen Abu Ali al-Hasan ibn al-Haytham]] (c. [[965]]-[[1040]]), also known as [[Alhazen]], developed a broad theory that explained vision, using [[geometry]] and [[anatomy]], which stated that each point on an illuminated area or object radiates light rays in every direction, but that only one ray from each point, which strikes the eye perpendicularly, can be seen. The other rays strike at different angles and are not seen.  He used the example of the [[pinhole camera]], which produces an inverted image, to support his argument.  This contradicted Ptolemy's theory of vision that objects are seen by rays of light emanating from the eyes. Alhazen held light rays to be streams of minute particles that travelled at a finite speed.  He improved [[Ptolemy]]'s theory of the refraction of light, and went on to discover the laws of refraction.
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He also carried out the first experiments on the dispersion of light into its constituent colors. His major work ''Kitab-at-Manazir'' was translated into [[Latin]] in the [[Middle Ages]], as well his book dealing with the colors of sunset. He dealt at length with the theory of various physical phenomena like shadows, eclipses, the rainbow. He also attempted to explain binocular vision, and gave a correct explanation of the apparent increase in size of the sun and the moon when near the horizon. Through these extensive researches on optics, is considered as the father of modern [[optics]].
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Al-Haytham also correctly argued that we see objects because the sun's rays of light, which he believed to be streams of tiny particles travelling in straight lines, are reflected from objects into our eyes. He understood that light must travel at a large but finite velocity, and that refraction is caused by the velocity being different in different substances. He also studied spherical and parabolic mirrors, and understood how refraction by a lens will allow images to be focused and magnification to take place. He understood mathematically why a spherical mirror produces aberration.
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===The 'plenum'===
 
[[René Descartes]] (1596-1650) held that light was a disturbance of the ''plenum'', the continuous substance of which the universe was composed.  In [[1637]] he published a theory of the refraction of light which wrongly assumed that light travelled faster in a denser medium, by analogy with the behaviour of sound waves.  Descartes' theory is often regarded as the forerunner of the wave theory of light.
 
[[René Descartes]] (1596-1650) held that light was a disturbance of the ''plenum'', the continuous substance of which the universe was composed.  In [[1637]] he published a theory of the refraction of light which wrongly assumed that light travelled faster in a denser medium, by analogy with the behaviour of sound waves.  Descartes' theory is often regarded as the forerunner of the wave theory of light.
  
=== Particle theory ===
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===Particle theory===
[[Pierre Gassendi]] (1592-1655), an atomist, proposed a [[particle]] theory of light which was published posthumously in the [[1660s]].  [[Isaac Newton]] studied Gassendi's work at an early age, and preferred his view to Descartes' theory of the ''plenum''.  He stated in his ''Hypothesis of Light'' of [[1675]] that light was composed of corpuscles (particles of matter) which were emitted in all directions from a source.  One of Newton's arguments against the wave nature of light was that waves were known to bend around obstacles, while light travelled only in straight lines.  He did, however, explain the phenomenon of the [[diffraction]] of light (which had been observed by [[Francesco Grimaldi]]) by allowing that a light particle could create a localised wave in the aether.
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[[Pierre Gassendi]] (1592-1655), an atomist, proposed a [[Wave-particle duality|particle theory]] of light which was published posthumously in the [[1660s]].  [[Isaac Newton]] studied Gassendi's work at an early age, and preferred his view to Descartes' theory of the ''plenum''.  He stated in his ''Hypothesis of Light'' of [[1675]] that light was composed of corpuscles (particles of matter) which were emitted in all directions from a source.  One of Newton's arguments against the wave nature of light was that waves were known to bend around obstacles, while light travelled only in straight lines.  He did, however, explain the phenomenon of the [[diffraction]] of light (which had been observed by [[Francesco Grimaldi]]) by allowing that a light particle could create a localised wave in the aether.
  
Newton's theory could be used to predict the [[reflection]] of light, but could only explain [[refraction]] by incorrectly assuming that light accelerated upon entering a denser [[medium]] because the [[gravity|gravitational]] pull was greater.  Newton published the final version of his theory in his ''[[Opticks]]'' of [[1704]].  His reputation helped the particle theory of light to dominate physics during the [[18th century]].
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Newton's theory could be used to predict the [[Reflection (physics)|reflection]] of light, but could only explain [[refraction]] by incorrectly assuming that light accelerated upon entering a denser [[Medium (optics)|medium]] because the [[gravity|gravitational]] pull was greater.  Newton published the final version of his theory in his ''[[Opticks]]'' of [[1704]].  His reputation helped the particle theory of light to dominate physics during the [[18th century]].
  
=== Wave theory ===
+
===Wave theory===
 
In the [[1660s]], [[Robert Hooke]] published a [[wave]] theory of light.  [[Christian Huygens]] worked out his own wave theory of light in 1678, and published it in his ''Treatise on light'' in [[1690]].  He proposed that light was emitted in all directions as a series of waves in a medium called the ''[[aether]]''.  As waves are not affected by gravity, it was assumed that they slowed down upon entering a denser medium.   
 
In the [[1660s]], [[Robert Hooke]] published a [[wave]] theory of light.  [[Christian Huygens]] worked out his own wave theory of light in 1678, and published it in his ''Treatise on light'' in [[1690]].  He proposed that light was emitted in all directions as a series of waves in a medium called the ''[[aether]]''.  As waves are not affected by gravity, it was assumed that they slowed down upon entering a denser medium.   
  
The wave theory predicted that light waves could interfere with each other like [[sound]] waves (as noted in the [[18th century]] by [[Thomas Young (scientist)|Thomas Young]]), and that light could be [[polarization|polarized]].  Young showed by means of a [[double-slit experiment|diffraction experiment]] that light behaved as waves.  He also proposed that different [[colour]]s were caused by different [[wavelength]]s of light, and explained colour vision in terms of three-coloured receptors in the eye.
+
The wave theory predicted that light waves could interfere with each other like [[sound]] waves (as noted in the [[18th century]] by [[Thomas Young (scientist)|Thomas Young]]), and that light could be [[polarization|polarized]].  Young showed by means of a [[double-slit experiment|diffraction experiment]] that light behaved as waves.  He also proposed that different [[color]]s were caused by different [[wavelength]]s of light, and explained color vision in terms of three-colored receptors in the eye.
  
 
Another supporter of the wave theory was [[Leonhard Euler|Euler]].  He argued in ''Nova theoria lucis et colorum'' ([[1746]]) that [[diffraction]] could more easily be explained by a wave theory.
 
Another supporter of the wave theory was [[Leonhard Euler|Euler]].  He argued in ''Nova theoria lucis et colorum'' ([[1746]]) that [[diffraction]] could more easily be explained by a wave theory.
  
Later, [[Augustin Jean Fresnel|Fresnel]] independently worked out his own wave theory of light, and presented it to the [[Académie des Sciences]] in [[1817]].  [[Simeon Poisson|Poisson]] added to Fresnel's mathematical work to produce a convincing argument in favour of the wave theory, helping to overturn Newton's corpuscular theory.
+
Later, [[Augustin Jean Fresnel|Fresnel]] independently worked out his own wave theory of light, and presented it to the [[Académie des Sciences]] in [[1817]].  Simeon Denis [[Simeon Poisson|Poisson]] added to Fresnel's mathematical work to produce a convincing argument in favour of the wave theory, helping to overturn Newton's corpuscular theory.
  
 
The weakness of the wave theory was that light waves, like sound waves, would need a medium for transmission.  A hypothetical substance called the [[luminiferous aether]] was proposed, but its existence was cast into strong doubt by the [[Michelson-Morley experiment]].
 
The weakness of the wave theory was that light waves, like sound waves, would need a medium for transmission.  A hypothetical substance called the [[luminiferous aether]] was proposed, but its existence was cast into strong doubt by the [[Michelson-Morley experiment]].
Line 125: Line 140:
 
Newton's corpuscular theory implied that light would travel faster in a denser medium, while the wave theory of Huygens and others implied the opposite.  At that time, the [[speed of light]] could not be measured accurately enough to decide which theory was correct.  The first to make a sufficiently accurate measurement was [[Léon Foucault]], in [[1850]].  His result supported the wave theory, and the classical particle theory was finally abandoned.
 
Newton's corpuscular theory implied that light would travel faster in a denser medium, while the wave theory of Huygens and others implied the opposite.  At that time, the [[speed of light]] could not be measured accurately enough to decide which theory was correct.  The first to make a sufficiently accurate measurement was [[Léon Foucault]], in [[1850]].  His result supported the wave theory, and the classical particle theory was finally abandoned.
  
=== Electromagnetic theory ===
+
===Electromagnetic theory===
In [[1845]], [[Faraday]] discovered that the angle of polarisation of a beam of light as it passed through a polarising material could be altered by a [[magnetic]] field, an effect now known as [[Faraday rotation]].  This was the first evidence that light was related to [[electromagnetism]].  Faraday proposed in [[1847]] that light was a high-frequency electromagnetic vibration, which could propagate even in the absence of a medium such as the aether.
+
In [[1845]], [[Faraday]] discovered that the angle of polarization of a beam of light as it passed through a polarizing material could be altered by a [[magnetic]] field, an effect now known as [[Faraday rotation]].  This was the first evidence that light was related to [[electromagnetism]].  Faraday proposed in [[1847]] that light was a high-frequency electromagnetic vibration, which could propagate even in the absence of a medium such as the ether.
  
 
Faraday's work inspired [[James Clerk Maxwell]] to study electromagnetic radiation and light.  Maxwell discovered that self-propagating electromagnetic waves would travel through space at a constant speed, which happened to be equal to the previously measured speed of light.  From this, Maxwell concluded that light was a form of electromagnetic radiation: he first stated this result in [[1862]] in ''On Physical Lines of Force''.  In [[1873]], he published ''[[A Treatise on Electricity and Magnetism]]'', which contained a full mathematical description of the behaviour of electric and magnetic fields, still known as [[Maxwell's equations]].  The technology of [[radio]] transmission was, and still is, based on this theory.   
 
Faraday's work inspired [[James Clerk Maxwell]] to study electromagnetic radiation and light.  Maxwell discovered that self-propagating electromagnetic waves would travel through space at a constant speed, which happened to be equal to the previously measured speed of light.  From this, Maxwell concluded that light was a form of electromagnetic radiation: he first stated this result in [[1862]] in ''On Physical Lines of Force''.  In [[1873]], he published ''[[A Treatise on Electricity and Magnetism]]'', which contained a full mathematical description of the behaviour of electric and magnetic fields, still known as [[Maxwell's equations]].  The technology of [[radio]] transmission was, and still is, based on this theory.   
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The constant speed of light predicted by Maxwell's equations contradicted the mechanical laws of motion that had been unchallenged since the time of [[Galileo Galilei|Galileo]], which stated that all speeds were relative to the speed of the observer.  A solution to this contradiction would later be found by [[Albert Einstein]].
 
The constant speed of light predicted by Maxwell's equations contradicted the mechanical laws of motion that had been unchallenged since the time of [[Galileo Galilei|Galileo]], which stated that all speeds were relative to the speed of the observer.  A solution to this contradiction would later be found by [[Albert Einstein]].
  
=== Particle theory revisited ===
+
===Particle theory revisited===
 
The wave theory was accepted until the late [[19th century]], when Einstein described the [[photoelectric effect]], by which light striking a surface caused electrons to change their [[momentum]], which indicated a particle-like nature of light.  This clearly contradicted the wave theory, and for years physicists tried in vain to resolve this contradiction.
 
The wave theory was accepted until the late [[19th century]], when Einstein described the [[photoelectric effect]], by which light striking a surface caused electrons to change their [[momentum]], which indicated a particle-like nature of light.  This clearly contradicted the wave theory, and for years physicists tried in vain to resolve this contradiction.
  
=== Quantum theory ===
+
===Quantum theory===
 
In 1900, [[Max Planck]] described [[quantum theory]], in which light is considered to be as a particle that could exist in discrete amounts of [[energy]] only.  These packets were called [[quantum|quanta]], and the particle of light was given the name [[photon]], to correspond with other particles being described around this time, such as the [[electron]] and [[proton]]. A
 
In 1900, [[Max Planck]] described [[quantum theory]], in which light is considered to be as a particle that could exist in discrete amounts of [[energy]] only.  These packets were called [[quantum|quanta]], and the particle of light was given the name [[photon]], to correspond with other particles being described around this time, such as the [[electron]] and [[proton]]. A
 
photon has an energy, E, proportional to its frequency, f, by
 
photon has an energy, E, proportional to its frequency, f, by
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:<math>E_f = hf = \frac{hc}{\lambda} \,\! </math>
 
:<math>E_f = hf = \frac{hc}{\lambda} \,\! </math>
  
where h is [[Planck's constant]], <math>\lambda</math> is the wavelength and c is the [[speed of light]].
+
where ''h'' is [[Planck's constant]], <math>\lambda</math> is the wavelength and ''c'' is the [[speed of light]].
  
 
As it originally stood, this theory did not explain the simultaneous wave-like nature of light, though Planck would later work on theories that did.  The [[Nobel Prize|Nobel Committee]] awarded Planck the [[Nobel Prize for Physics|Physics Prize]] in [[1918]] for his part in the founding of quantum theory.
 
As it originally stood, this theory did not explain the simultaneous wave-like nature of light, though Planck would later work on theories that did.  The [[Nobel Prize|Nobel Committee]] awarded Planck the [[Nobel Prize for Physics|Physics Prize]] in [[1918]] for his part in the founding of quantum theory.
  
=== Wave-particle duality ===
+
===Wave-particle duality===
The modern theory that explains the nature of light is [[wave-particle duality]], described by [[Albert Einstein]] in the early 1900s, based on his work on the photoelectric effect and Planck's results.  Einstein determined that the energy of a photon is proportional to its [[frequency]].  More generally, the theory states that everything has both a particle nature, and a wave nature, and various experiments can be done to bring out one or the other.  The particle nature is more easily discerned if an object has a large mass, so it took until an experiment by [[Louis de Broglie]] in 1924 to realise that [[electrons]] also exhibited wave-particle duality.  Einstein received the Nobel Prize in [[1921]] for his work with the wave-particle duality on photons, and de Broglie followed in [[1929]] for his extension to other particles.
+
The modern theory that explains the nature of light is [[wave-particle duality]], described by [[Albert Einstein]] in the early 1900s, based on his work on the photoelectric effect and Planck's results.  Einstein determined that the energy of a photon is proportional to its [[frequency]].  More generally, the theory states that everything has both a particle nature and a wave nature, and various experiments can be done to bring out one or the other.  The particle nature is more easily discerned if an object has a large mass, so it took until an experiment by [[Louis de Broglie]] in 1924 to realise that [[electrons]] also exhibited wave-particle duality.  Einstein received the Nobel Prize in [[1921]] for his work with the wave-particle duality on photons, and de Broglie followed in [[1929]] for his extension to other particles.
  
 
===A light wave===
 
===A light wave===
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The electric and magnetic fields are perpendicular to the direction of travel and to each other. This picture depicts a very special case, linearly polarized light. See [[Polarization]] for a description of the general case and an explanation of linear polarization.  
 
The electric and magnetic fields are perpendicular to the direction of travel and to each other. This picture depicts a very special case, linearly polarized light. See [[Polarization]] for a description of the general case and an explanation of linear polarization.  
  
While the above statements about the relations of the electric and magnetic fields are always true, the subtle difference in the general case is that the direction and amplitude of the magnetic (or electric) field can vary, in one place, with time, or, in one instant, can vary along the direction of propagation.
+
While these relations of the electric and magnetic fields are always true, the subtle difference in the general case is that the direction and amplitude of the magnetic (or electric) field can vary, in one place, with time, or, in one instant, can vary along the direction of propagation.
 +
 
 +
==References==
 +
<div class="references-small">
 +
*[[Max Muller|M. Muller]]. ''Rig-Veda-Samhita together with the Commentary of Sayana'', [[Oxford University Press]], [[London]], 1890.
 +
*B. K. Matilal. ''Nyaya-Vaisesika'', Otto Harrassowitz, Wiesbaden, 1977.
 +
*K. H. Potter, ''Indian Metaphysics and Epistemology'', [[Princeton University Press]], [[Princeton, New Jersey|Princeton]], 1977.
 +
*G. J. Larson and R. S. Bhattacharya. ''Samkhya: A Dualist Tradition in Indian Philosophy'', Princeton University Press, Princeton, 1987.
 +
*S. S. De. ''In Issues in Vedic Astronomy and Astrology'', Motilal Banarsidass, 1992.
 +
*P. V. Vartak. ''Scientific Knowledge in the Vedas'', Nag Publishers, 1995.
 +
*[[Subhash Kak|S. Kak]]. "The Speed of Light and {{unicode|Purāṇic}} Cosmology". In T. R. N. Rao and S. Kak, ''Computing Science in Ancient India,'' pages 80&ndash;90. USL Press, Lafayette, 1998. Available as [http://uk.arxiv.org/abs/physics/9804020 e-print physics/9804020] on the [[arXiv]].
 +
</div>
  
 
==See also==
 
==See also==
 
 
{{commons|Light}}
 
{{commons|Light}}
*[[Color temperature]]
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*[[Colour temperature]]
 
*[[Huygens' principle]]
 
*[[Huygens' principle]]
 
*[[Fermat's principle]]
 
*[[Fermat's principle]]
 
*[[International Commission on Illumination]]
 
*[[International Commission on Illumination]]
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*[[Light beam]] - in particular about light beams visible from the side
 
*[[Light pollution]]
 
*[[Light pollution]]
 
*[[Lighting]]
 
*[[Lighting]]
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Revision as of 20:23, 9 June 2006

Prism splitting light

Light is electromagnetic radiation with a wavelength that is visible to the eye (visible light) or, in a technical or scientific context, electromagnetic radiation of any wavelength. The three basic dimensions of light (i.e., all electromagnetic radiation) are:

  • Intensity (or amplitude), which is related to the human perception of brightness of the light,
  • Frequency (or wavelength), perceived by humans as the color of the light, and
  • Polarization (or angle of vibration), which is not perceptible by humans under ordinary circumstances.

Due to the wave-particle duality of matter, light simultaneously exhibits properties of both waves and particles. The precise nature of light is one of the key questions of modern physics.

Visible electromagnetic radiation

Speed of light

The speed of light in a vacuum is exactly 299,792,458 metres per second (fixed by definition). Although some people speak of the "velocity of light", the word velocity is usually reserved for vector quantities, which have a direction.

Some scholars have conjectured that the speed of light was first known in India, based on a statement by Sayana (c. 1315-1387). Max Muller's translation of Sayana's commentary on the Rig Veda states: "Thus it is remembered: [O Sun] you who traverse 2202 yojanas in half a nimesa." This corresponds to a speed of about 302,073 km/s, which is close to the speed of light (299,792 km/s). This statement also occurs in Bhatta Bhaskara's earlier commentary on the Taittiriya Brahmana. There is still much debate on whether Sayana was estimating the speed of light or overestimating the speed of the Sun, since he didn't make it clear which he was referring to, nor did he give any methods for his estimate.

The speed of light has been measured many times, by many physicists. The best early measurement in Europe is by Ole Rømer, a Danish physicist, in 1676. By observing the motions of Jupiter and one of its moons, Io, with a telescope, and noting discrepancies in the apparent period of Io's orbit, Rømer calculated that light takes about 18 minutes to traverse the diameter of Earth's orbit. Had he known the diameter of the orbit in kilometers (which he didn't) he would have deduced a speed of 227,000 kilometres per second (approximately 141,050 miles per second).

The first successful measurement of the speed of light in Europe using an earthbound apparatus was carried out by Hippolyte Fizeau in 1849. Fizeau directed a beam of light at a mirror several thousand metres away, and placed a rotating cog wheel in the path of the beam from the source to the mirror and back again. At a certain rate of rotation, the beam could pass through one gap in the wheel on the way out and the next gap on the way back. Knowing the distance to the mirror, the number of teeth on the wheel, and the rate of rotation, Fizeau measured the speed of light as 313,000 kilometres per second.

Léon Foucault used rotating mirrors to obtain a value of 298,000 km/s (about 185,000 miles/s) in 1862. Albert A. Michelson conducted experiments on the speed of light from 1877 until his death in 1931. He refined Foucault's results in 1926 using improved rotating mirrors to measure the time it took light to make a round trip from Mt. Wilson to Mt. San Antonio in California. The precise measurements yielded a speed of 186,285 mi/s (299,796 km/s [1,079,265,600 km/h]). In daily use, the figures are rounded off to 300,000 km/s and 186,000 miles/s.

Refraction

Main article: Refraction

All light propagates at a finite speed. Even moving observers always measure the same value of c, the speed of light in vacuum, as c = 299,792,458 metres per second (186,282.397 miles per second). When light passes through a transparent substance, such as air, water or glass, its speed is reduced, and it undergoes refraction. The reduction of the speed of light in a denser material can be indicated by the refractive index, n, which is defined as:

Thus, n = 1 in a vacuum and n > 1 in matter.

When a beam of light enters a medium from vacuum or another medium, it keeps the same frequency and changes its wavelength. If the incident beam is not orthogonal to the edge between the media, the direction of the beam will change. Refraction of light by lenses is used to focus light in magnifying glasses, spectacles and contact lenses, microscopes and refracting telescopes.

Optics

The study of light and the interaction of light and matter is termed optics. The observation and study of optical phenomena such as rainbows offers many clues as to the nature of light as well as much enjoyment.

Colour and wavelength

The different wavelengths are detected by the human eye and then interpreted by the brain as colours, ranging from red at the longest wavelengths of about 700 nm to violet at the shortest wavelengths of about 400 nm. The intervening frequencies are seen as orange, yellow, green, and blue.



The wavelengths of the electromagnetic spectrum immediately outside the range that the human eye is able to perceive are called ultraviolet (UV) at the short wavelength (high frequency) end and infrared (IR) at the long wavelength (low frequency) end. Some animals, such as bees, can see UV radiation while others, such as pit viper snakes, can see infrared light.

UV radiation is not normally directly perceived by humans except in a very delayed fashion, as overexposure of the skin to UV light can cause sunburn, or skin cancer, and underexposure can cause vitamin D deficiency. However, because UV is a higher frequency radiation than visible light, it very easily can cause materials to fluoresce visible light.

Cameras that can detect IR and convert it to light are called, depending on their application, night-vision cameras or infrared cameras. These are different from image intensifier cameras, which only amplify available visible light.

When intense radiation (of any frequency) is absorbed in the skin, it causes heating which can be felt. Since hot objects are strong sources of infrared radiation, IR radiation is commonly associated with this sensation. Any intense radiation that can be absorbed in the skin will have the same effect, however.

Measurement of light

The following quantities and units are used to measure the quantity or "brightness" of light. Template:SI light units Template:SI radiometry units

Light can also be characterised by:

Light sources

Sunlight scattered by smoke

There are many sources of light. The most common light sources are thermal: a body at a given temperature emits a characteristic spectrum of black body radiation. Examples include sunlight (the radiation emitted by the chromosphere of the Sun at around 6,000 K peaks in the visible region of the electromagnetic spectrum), incandescent light bulbs (which emit only around 10% of their energy as visible light and the remainder as infrared), and glowing solid particles in flames. The peak of the blackbody spectrum is in the infrared for relatively cool objects like human beings. As the temperature increases, the peak shifts to shorter wavelengths, producing first a red glow, then a white one, and finally a blue color as the peak moves out of the visible part of the spectrum and into the ultraviolet. These colors can be seen when metal is heated to "red hot" or "white hot". The blue color is most commonly seen in a gas flame or a welder's torch.

Atoms emit and absorb light at characteristic energies. This produces "emission lines" in the spectrum of each atom. Emission can be spontaneous, as in light-emitting diodes, gas discharge lamps (such as neon lamps and neon signs, mercury-vapor lamps, etc.), and flames (light from the hot gas itself—so, for example, sodium in a gas flame emits characteristic yellow light). Emission can also be stimulated, as in a laser or a microwave maser.

Acceleration of a free charged particle, such as an electron, can produce visible radiation: cyclotron radiation, synchrotron radiation, and bremsstrahlung radiation are all examples of this. Particles moving through a medium faster than the speed of light in that medium can produce visible Cherenkov radiation.

Certain chemicals produce visible radiation by chemoluminescence. In living things, this process is called bioluminescence. For example, fireflies produce light by this means, and boats moving through water can disturb plankton which produce a glowing wake.

Certain substances produce light when they are illuminated by more energetic radiation, a process known as fluorescence. This is used in fluorescent lights. Some substances emit light slowly after excitation by more energetic radiation. This is known as phosphorescence.

Phosphorescent materials can also be excited by bombarding them with subatomic particles. Cathodoluminescence is one example of this. This mechanism is used in cathode ray tube televisions.

Certain other mechanisms can produce light:

  • scintillation
    • scintillator
  • electroluminescence
  • sonoluminescence
  • triboluminescence
  • radioactive decay
  • particle-antiparticle annihilation

Theories about light

Indian theories

In ancient India, the philosophical schools of Samkhya and Vaisheshika, from around the 6th–5th century B.C.E., developed theories on light. According to the Samkhya school, light is one of the five fundamental "subtle" elements (tanmatra) out of which emerge the gross elements. The atomicity of these elements is not specifically mentioned and it appears that they were actually taken to be continuous.

On the other hand, the Vaisheshika school gives an atomic theory of the physical world on the non-atomic ground of ether, space and time. (See Indian atomism.) The basic atoms are those of earth (prthivı), water (apas), fire (tejas), and air (vayu), that should not be confused with the ordinary meaning of these terms. These atoms are taken to form binary molecules that combine further to form larger molecules. Motion is defined in terms of the movement of the physical atoms and it appears that it is taken to be non-instantaneous. Light rays are taken to be a stream of high velocity of tejas (fire) atoms. The particles of light can exhibit different characteristics depending on the speed and the arrangements of the tejas atoms.

Later in 499 C.E., Aryabhata, who proposed a heliocentric solar system of gravitation in his Aryabhatiya, wrote that the planets and the Moon do not have their own light but reflect the light of the Sun.

The Indian Buddhists, such as Dignāga in the 5th century and Dharmakirti in the 7th century, developed a type of atomism that is a philosophy about reality being composed of atomic entities that are momentary flashes of light or energy. They viewed light as being an atomic entity equivalent to energy, similar to the modern concept of photons, though they also viewed all matter as being composed of these light/energy particles.

Greek and Hellenistic theories

In the fifth century B.C.E., Empedocles postulated that everything was composed of four elements; fire, air, earth and water. He believed that Aphrodite made the human eye out of the four elements and that she lit the fire in the eye which shone out from the eye making sight possible. If this were true, then one could see during the night just as well as during the day, so Empedocles postulated an interaction between rays from the eyes and rays from a source such as the sun.

In about 300 B.C.E., Euclid wrote Optica, in which he studied the properties of light. Euclid postulated that light travelled in straight lines and he described the laws of reflection and studied them mathematically. He questioned that sight is the result of a beam from the eye, for he asks how one sees the stars immediately, if one closes ones eyes, then opens them at night. Of course if the beam from the eye travels infinitely fast this is not a problem.

In 55 B.C.E., Lucretius, a Roman who carried on the ideas of earlier Greek atomists, wrote:

"The light and heat of the sun; these are composed of minute atoms which, when they are shoved off, lose no time in shooting right across the interspace of air in the direction imparted by the shove." - On the nature of the Universe

Despite being remarkably similar to how we think of light today, Lucretius's views were not generally accepted and light was still theorized as emanating from the eye.

Ptolemy (c. 2nd century CE) wrote about the refraction of light, and developed a theory of vision that objects are seen by rays of light emanating from the eyes.

Optical theory

The Persian scientist Alhazen Abu Ali al-Hasan ibn al-Haytham (c. 965-1040), also known as Alhazen, developed a broad theory that explained vision, using geometry and anatomy, which stated that each point on an illuminated area or object radiates light rays in every direction, but that only one ray from each point, which strikes the eye perpendicularly, can be seen. The other rays strike at different angles and are not seen. He used the example of the pinhole camera, which produces an inverted image, to support his argument. This contradicted Ptolemy's theory of vision that objects are seen by rays of light emanating from the eyes. Alhazen held light rays to be streams of minute particles that travelled at a finite speed. He improved Ptolemy's theory of the refraction of light, and went on to discover the laws of refraction.

He also carried out the first experiments on the dispersion of light into its constituent colors. His major work Kitab-at-Manazir was translated into Latin in the Middle Ages, as well his book dealing with the colors of sunset. He dealt at length with the theory of various physical phenomena like shadows, eclipses, the rainbow. He also attempted to explain binocular vision, and gave a correct explanation of the apparent increase in size of the sun and the moon when near the horizon. Through these extensive researches on optics, is considered as the father of modern optics.

Al-Haytham also correctly argued that we see objects because the sun's rays of light, which he believed to be streams of tiny particles travelling in straight lines, are reflected from objects into our eyes. He understood that light must travel at a large but finite velocity, and that refraction is caused by the velocity being different in different substances. He also studied spherical and parabolic mirrors, and understood how refraction by a lens will allow images to be focused and magnification to take place. He understood mathematically why a spherical mirror produces aberration.

The 'plenum'

René Descartes (1596-1650) held that light was a disturbance of the plenum, the continuous substance of which the universe was composed. In 1637 he published a theory of the refraction of light which wrongly assumed that light travelled faster in a denser medium, by analogy with the behaviour of sound waves. Descartes' theory is often regarded as the forerunner of the wave theory of light.

Particle theory

Pierre Gassendi (1592-1655), an atomist, proposed a particle theory of light which was published posthumously in the 1660s. Isaac Newton studied Gassendi's work at an early age, and preferred his view to Descartes' theory of the plenum. He stated in his Hypothesis of Light of 1675 that light was composed of corpuscles (particles of matter) which were emitted in all directions from a source. One of Newton's arguments against the wave nature of light was that waves were known to bend around obstacles, while light travelled only in straight lines. He did, however, explain the phenomenon of the diffraction of light (which had been observed by Francesco Grimaldi) by allowing that a light particle could create a localised wave in the aether.

Newton's theory could be used to predict the reflection of light, but could only explain refraction by incorrectly assuming that light accelerated upon entering a denser medium because the gravitational pull was greater. Newton published the final version of his theory in his Opticks of 1704. His reputation helped the particle theory of light to dominate physics during the 18th century.

Wave theory

In the 1660s, Robert Hooke published a wave theory of light. Christian Huygens worked out his own wave theory of light in 1678, and published it in his Treatise on light in 1690. He proposed that light was emitted in all directions as a series of waves in a medium called the aether. As waves are not affected by gravity, it was assumed that they slowed down upon entering a denser medium.

The wave theory predicted that light waves could interfere with each other like sound waves (as noted in the 18th century by Thomas Young), and that light could be polarized. Young showed by means of a diffraction experiment that light behaved as waves. He also proposed that different colors were caused by different wavelengths of light, and explained color vision in terms of three-colored receptors in the eye.

Another supporter of the wave theory was Euler. He argued in Nova theoria lucis et colorum (1746) that diffraction could more easily be explained by a wave theory.

Later, Fresnel independently worked out his own wave theory of light, and presented it to the Académie des Sciences in 1817. Simeon Denis Poisson added to Fresnel's mathematical work to produce a convincing argument in favour of the wave theory, helping to overturn Newton's corpuscular theory.

The weakness of the wave theory was that light waves, like sound waves, would need a medium for transmission. A hypothetical substance called the luminiferous aether was proposed, but its existence was cast into strong doubt by the Michelson-Morley experiment.

Newton's corpuscular theory implied that light would travel faster in a denser medium, while the wave theory of Huygens and others implied the opposite. At that time, the speed of light could not be measured accurately enough to decide which theory was correct. The first to make a sufficiently accurate measurement was Léon Foucault, in 1850. His result supported the wave theory, and the classical particle theory was finally abandoned.

Electromagnetic theory

In 1845, Faraday discovered that the angle of polarization of a beam of light as it passed through a polarizing material could be altered by a magnetic field, an effect now known as Faraday rotation. This was the first evidence that light was related to electromagnetism. Faraday proposed in 1847 that light was a high-frequency electromagnetic vibration, which could propagate even in the absence of a medium such as the ether.

Faraday's work inspired James Clerk Maxwell to study electromagnetic radiation and light. Maxwell discovered that self-propagating electromagnetic waves would travel through space at a constant speed, which happened to be equal to the previously measured speed of light. From this, Maxwell concluded that light was a form of electromagnetic radiation: he first stated this result in 1862 in On Physical Lines of Force. In 1873, he published A Treatise on Electricity and Magnetism, which contained a full mathematical description of the behaviour of electric and magnetic fields, still known as Maxwell's equations. The technology of radio transmission was, and still is, based on this theory.

The constant speed of light predicted by Maxwell's equations contradicted the mechanical laws of motion that had been unchallenged since the time of Galileo, which stated that all speeds were relative to the speed of the observer. A solution to this contradiction would later be found by Albert Einstein.

Particle theory revisited

The wave theory was accepted until the late 19th century, when Einstein described the photoelectric effect, by which light striking a surface caused electrons to change their momentum, which indicated a particle-like nature of light. This clearly contradicted the wave theory, and for years physicists tried in vain to resolve this contradiction.

Quantum theory

In 1900, Max Planck described quantum theory, in which light is considered to be as a particle that could exist in discrete amounts of energy only. These packets were called quanta, and the particle of light was given the name photon, to correspond with other particles being described around this time, such as the electron and proton. A photon has an energy, E, proportional to its frequency, f, by

where h is Planck's constant, is the wavelength and c is the speed of light.

As it originally stood, this theory did not explain the simultaneous wave-like nature of light, though Planck would later work on theories that did. The Nobel Committee awarded Planck the Physics Prize in 1918 for his part in the founding of quantum theory.

Wave-particle duality

The modern theory that explains the nature of light is wave-particle duality, described by Albert Einstein in the early 1900s, based on his work on the photoelectric effect and Planck's results. Einstein determined that the energy of a photon is proportional to its frequency. More generally, the theory states that everything has both a particle nature and a wave nature, and various experiments can be done to bring out one or the other. The particle nature is more easily discerned if an object has a large mass, so it took until an experiment by Louis de Broglie in 1924 to realise that electrons also exhibited wave-particle duality. Einstein received the Nobel Prize in 1921 for his work with the wave-particle duality on photons, and de Broglie followed in 1929 for his extension to other particles.

A light wave

File:Light-wave.png
This is a light wave frozen in time and shows the two components of light; an electric field and a magnetic field that oscillate perpendicular to each other and to the direction of motion (a transverse wave).

The electric and magnetic fields are perpendicular to the direction of travel and to each other. This picture depicts a very special case, linearly polarized light. See Polarization for a description of the general case and an explanation of linear polarization.

While these relations of the electric and magnetic fields are always true, the subtle difference in the general case is that the direction and amplitude of the magnetic (or electric) field can vary, in one place, with time, or, in one instant, can vary along the direction of propagation.

References
ISBN links support NWE through referral fees

  • M. Muller. Rig-Veda-Samhita together with the Commentary of Sayana, Oxford University Press, London, 1890.
  • B. K. Matilal. Nyaya-Vaisesika, Otto Harrassowitz, Wiesbaden, 1977.
  • K. H. Potter, Indian Metaphysics and Epistemology, Princeton University Press, Princeton, 1977.
  • G. J. Larson and R. S. Bhattacharya. Samkhya: A Dualist Tradition in Indian Philosophy, Princeton University Press, Princeton, 1987.
  • S. S. De. In Issues in Vedic Astronomy and Astrology, Motilal Banarsidass, 1992.
  • P. V. Vartak. Scientific Knowledge in the Vedas, Nag Publishers, 1995.
  • S. Kak. "The Speed of Light and Purāṇic Cosmology". In T. R. N. Rao and S. Kak, Computing Science in Ancient India, pages 80–90. USL Press, Lafayette, 1998. Available as e-print physics/9804020 on the arXiv.

See also

Commons
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