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	<id>http://cleanenergywiki.org/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=24.19.10.162</id>
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	<updated>2026-04-23T21:58:10Z</updated>
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	<entry>
		<id>http://cleanenergywiki.org/index.php?title=Optical_Fibers&amp;diff=4437</id>
		<title>Optical Fibers</title>
		<link rel="alternate" type="text/html" href="http://cleanenergywiki.org/index.php?title=Optical_Fibers&amp;diff=4437"/>
		<updated>2009-08-27T00:34:57Z</updated>

		<summary type="html">&lt;p&gt;24.19.10.162: /* Circular Dielectric Waveguides */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;table id=&amp;quot;toc&amp;quot; style=&amp;quot;width: 100%&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: center; width: 33%&amp;quot;&amp;gt;[[Main_Page#Optical Fibers, Waveguides, and Lasers|Return to Optical Fibers, Waveguides, and Lasers Menu]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: right; width: 33%&amp;quot;&amp;gt;[[Total Internal Reflection|Next Topic]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Optical Fiber ==&lt;br /&gt;
Optical fibers are transparent glass or plastic tubes that carry information encoded light. Other fiber optic cables are used to transmit intense light to pump lasers or for remote imaging such as a boroscope.&lt;br /&gt;
&lt;br /&gt;
See also Wikipedia [http://en.wikipedia.org/wiki/Optic_fiber Optic Fiber]&lt;br /&gt;
=== Fiber Requirements ===&lt;br /&gt;
&lt;br /&gt;
Visible light has a frequency of 10&amp;lt;sup&amp;gt;14&amp;lt;/sup&amp;gt; Hz.  A light signal can be modulated at much higher frequencies than either radio or micowave. The movement from electrons to photonics is driven by the desire to create communication channels using high frequency carriers and which have extremely high information content. This requires that light be guided and controlled in precise ways, over long distances. Optical fibers can carry data at a rate of gigabytes per second, or the equivalent of several thousand phone conversations in parallel. The extraordinary transparency of optical fibers materials makes it possible to propagate light sometimes hundreds of miles without amplification.&lt;br /&gt;
&lt;br /&gt;
=== History ===&lt;br /&gt;
&lt;br /&gt;
In 1870 Tyndall demonstrated that light could be guided within a water jet as a result of total internal reflection.&lt;br /&gt;
&lt;br /&gt;
In  1954 it was proposed to create a cladded dielectric waveguide that has a core with a higher refractive index than the cladding.&lt;br /&gt;
&lt;br /&gt;
In the mid 1960s research turned to building a communication system based on circular dielectric waveguides.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Circular Dielectric Waveguides ===&lt;br /&gt;
&lt;br /&gt;
[[Image:550px-Optical-fibre.svg.png|thumb|300px|Light is reflected inside an optical fiber]]&lt;br /&gt;
A circular dielectric waveguide or fiber optic has an internal core that has a lower index of refraction than the cladding. &lt;br /&gt;
&lt;br /&gt;
At a certain diameter there is an angle such that there is total internal reflection. We can use mathematics to determine how to improve the material for less loss over longer distances. &lt;br /&gt;
&lt;br /&gt;
The plane of incidence is a plane containing both the axis of the beam and the normal (perpendicular line) to the interface. For the flat drawing shown that would be the plane of the screen. A wave vector can be decomposed into a component that is perpendicular to the plane and a component that is parallel to the plane.&lt;br /&gt;
&lt;br /&gt;
For an electric field vector that is perpendicular to the plane of incidence the phase is 2 &amp;amp;psi; where:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;tan \psi = \frac {[sin^2 \theta_i – (n_2/n_1)^ 2 ]^{1/2}}   {cos \theta_i}\,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For an electric field vector that is parallel to the plane of incidence the phase change is 2 &amp;amp;delta; where &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;tan \delta  = (n_1/n_2)^2 tan \psi\,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So as a function of the index of refraction there is change in phase of the reflected beam as it interacts with the material. This will be critical in determining how a beam propagates.&lt;br /&gt;
&lt;br /&gt;
Here is an example using a glass air interface. The glass (n&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) has an index of refraction of 1.5 and air (n&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is 1.0 and the critical angle (&amp;amp;theta;&amp;lt;sub&amp;gt; c&amp;lt;/sub&amp;gt;) is 41.8 deg. The graph shows that phase change increases as the beam becomes more parallel with the interface.&lt;br /&gt;
 &lt;br /&gt;
All the energy in the beam is reflected when theta i &amp;gt; &amp;amp;theta;&amp;lt;sub&amp;gt; c&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Image:Phase_para_normal.png|thumb|300px|Above the critical angle increasing angle of incidence leads to greater phase change]]&lt;br /&gt;
&lt;br /&gt;
In the second medium the electric field amplitude decays exponentially with distance away from the boundary. The part of the field in the second medium is referred to as the '''evanescent field'''.  The evanescent field can be measured using thin film techniques because the exponential decay means it does not penetrate far into the medium.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br clear='all'&amp;gt;&lt;br /&gt;
&amp;lt;table id=&amp;quot;toc&amp;quot; style=&amp;quot;width: 100%&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: center; width: 33%&amp;quot;&amp;gt;[[Main_Page#Optical Fibers, Waveguides, and Lasers|Return to Optical Fibers, Waveguides, and Lasers Menu]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: right; width: 33%&amp;quot;&amp;gt;[[Total Internal Reflection|Next Topic]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;/div&gt;</summary>
		<author><name>24.19.10.162</name></author>
	</entry>
	<entry>
		<id>http://cleanenergywiki.org/index.php?title=Chromaticity&amp;diff=4436</id>
		<title>Chromaticity</title>
		<link rel="alternate" type="text/html" href="http://cleanenergywiki.org/index.php?title=Chromaticity&amp;diff=4436"/>
		<updated>2009-08-27T00:33:28Z</updated>

		<summary type="html">&lt;p&gt;24.19.10.162: /* External Links */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;table id=&amp;quot;toc&amp;quot; style=&amp;quot;width: 100%&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: left; width: 33%&amp;quot;&amp;gt;[[Color|Previous Topic]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: center; width: 33%&amp;quot;&amp;gt;[[Main_Page#Luminescence and Color|Return to Luminescence Menu]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Chromaticity ==&lt;br /&gt;
&lt;br /&gt;
Engineers and designers have very specific requirements for light emitting and light absorbing materials. They frequently use a color measurement system called tristimulus to precisely specify any possible color, even those that can not be described with a simple wavelength.&lt;br /&gt;
&lt;br /&gt;
=== Tristimulus measurement and chromaticity diagrams ===&lt;br /&gt;
&lt;br /&gt;
The tristimulus color measurement system is based on visually matching a color under standardized conditions against the three primary colors, red, green, and blue; the three results are expressed as X, Y, and Z, respectively, and are called '''tristimulus''' values &lt;br /&gt;
&lt;br /&gt;
These values specify not only color but also visually perceived reflectance, since they are calculated in such a way that the Y value equals a sample's reflectivity (39.1 percent in this example) when visually compared to a standard white surface by a standard (average) viewer under average daylight.&lt;br /&gt;
&lt;br /&gt;
The tristimulus values of the emerald-green pigment of Figure 6 are X = 22.7, Y = 39.1, and Z = 31.0[[Image:Emeraldabsorb.jpg|thumb|200px|Reflectance of emerald green color]]&lt;br /&gt;
&lt;br /&gt;
The tristimulus values can also be used to determine the visually perceived dominant spectral wavelength (which is related to the hue) of a given sample; the dominant wavelength of the emerald-green pigment is 511.9 nm:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
it is based on the values x, y, and z, &lt;br /&gt;
&lt;br /&gt;
Where&lt;br /&gt;
&lt;br /&gt;
'''x = X/(X + Y + Z)'''&lt;br /&gt;
&lt;br /&gt;
'''y = Y/(X + Y + Z)'''&lt;br /&gt;
&lt;br /&gt;
'''z = Z/(X + Y + Z)'''&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br clear='all'&amp;gt;&lt;br /&gt;
[[Image:Cie_chromaticity_diagram_wavelength.png|thumb|300px|]]&lt;br /&gt;
Note that x + y + z = 1; thus if two values are known, the third can always be calculated and the z value is usually omitted thus, the x and y values together constitute the chromaticity of a sample light and dark colors that have the same chromaticity (and are therefore plotted at the same point on the two-dimensional chromaticity diagram) can be distinguished in a third dimension (by their luminance or visually perceived brightness).&lt;br /&gt;
&lt;br /&gt;
White light is x= 1/3, y = 1/3 and z= 1/3. This is achromatic point. Pure grays and black are the same hue as white light but vary only in the magnitude of their luminance. Occasionally colors will be also be described using luminance as well.&lt;br /&gt;
&lt;br /&gt;
So for the goal of LED makers is to make a white light with x and y values close to 1/3.&lt;br /&gt;
&lt;br /&gt;
Around the horseshoe shaped periphery are the pure saturated colors , beginning with 400nm (violet) and going around to 700 nm (red). Those are the colors of the visible spectrum.  The straight line across the bottom are  colors that come from the non-spectral mixing of violet and red, they do not correspond to a single wavelength.&lt;br /&gt;
&amp;lt;br clear='all'&amp;gt;&lt;br /&gt;
[[Image:300px-CIExy1931_twocolors.png|thumb|300px|]]&lt;br /&gt;
&lt;br /&gt;
=== Plotting CIE values ===&lt;br /&gt;
&lt;br /&gt;
By plotting the calculated x = 0.245 and y = 0.421 of the emerald-green pigment at point E on the chromaticity diagram and extending a line through it from the achromatic point W to the saturated spectral boundary, it is possible to determine the dominant wavelength of the pigment color, 511.9 nm. Emerald green is not a pure color. But it can be made by mixing the pure color with wavelength 511.9nm  with white light.&lt;br /&gt;
&lt;br /&gt;
The color of the pigment is the visual equivalent of adding white light and light of 511.9 nm in amounts proportional to the lengths '''n''' (the distance between points '''E''' and '''W''') and '''m''' (the distance between '''E''' and the point of the dominant wavelength) in the figure. The saturation or purity equals 100n/(m + n) percent - in this case, 22.8 percent. A purity of 100 percent corresponds to a pure saturated spectral color and 0 percent to the achromatic colors (white, gray, and black)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Another example, a red apple marked '''R''' on the diagram. If you connect the line through '''w''' and '''R''' it intersects the bottom line which are not pure spectral colors. In this case this shade of red must be defined in terms of the complementary color on the opposite side of the achromatic point.&lt;br /&gt;
&lt;br /&gt;
The dominant color designation is then obtained by extrapolating the line in the opposite direction to a saturated spectral color it is given as &amp;quot;complementary dominant wavelength 495 nm&amp;quot; or 495c. The color of this apple is therefore the visual equivalent of a mixture of white light and the 495c saturated purple-red in the intensity ratio of the distances p to q shown in the figure with a purity of 100p/(p + q) percent.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br clear='all'&amp;gt;&lt;br /&gt;
=== Incandescent light sources ===&lt;br /&gt;
&lt;br /&gt;
[[Image:533px-PlanckianLocus.png|thumb|300px|]]&lt;br /&gt;
Light from incandescent sources falls on the solid curve marked with temperatures in this figure, following the sequence saturated red to saturated orange to unsaturated yellow to white to unsaturated bluish white for an infinite temperature.&lt;br /&gt;
&lt;br /&gt;
The points A, B, and C on the curve are CIE standard illuminants that approximate, respectively, a 100-watt incandescent filament lamp at a color temperature of about 2,850 K, noon sunlight (about 4,800 K), and average daylight (about 6,500 K)&lt;br /&gt;
&lt;br /&gt;
The color of daylight changes over the course of a day. LED designers could make the color of their devices change during the day to better match the daylight experience. Some white lights feel “warmer “ or “colder “depending on the color balance. LEDs will have the same descriptives.&lt;br /&gt;
&lt;br /&gt;
== External Links ==&lt;br /&gt;
&lt;br /&gt;
[http://hyperphysics.phy-astr.gsu.edu/hbase/vision/colper.html#c2 Hyperphysics materials about chromaticity]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br clear='all'&amp;gt;&lt;br /&gt;
&amp;lt;table id=&amp;quot;toc&amp;quot; style=&amp;quot;width: 100%&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: left; width: 33%&amp;quot;&amp;gt;[[Color|Previous Topic]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;td style=&amp;quot;text-align: center; width: 33%&amp;quot;&amp;gt;[[Main_Page#Luminescence and Color|Return to Luminescence Menu]]&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;/div&gt;</summary>
		<author><name>24.19.10.162</name></author>
	</entry>
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