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combination of light refraction and reflection, using materials with differing<br />

refraction indices. The refraction index determines how <strong>the</strong> wavelength of light is<br />

bent when it passes through a substance and also <strong>the</strong> rate of pho<strong>to</strong>n passage<br />

through <strong>the</strong> substance. Though copper and fiber cabling both transport data at <strong>the</strong><br />

same rate (0.69 percent of <strong>the</strong> speed of light), <strong>the</strong> difference between <strong>the</strong> two is <strong>the</strong><br />

amount of useable bandwidth, due <strong>to</strong> fiber optic's low attenuation rating. Fiber optic<br />

cable suffers minimal signal loss in <strong>the</strong> form of actual resistance, because pho<strong>to</strong>ns<br />

instead of electrons are used. This results in a more effective use of <strong>the</strong> transmission<br />

medium. The actual amount of bandwidth available for transmission is determined<br />

by <strong>the</strong> width of <strong>the</strong> light source and <strong>the</strong> rise and fall rate of <strong>the</strong> light. The narrower<br />

<strong>the</strong> light wavelength and <strong>the</strong> faster <strong>the</strong> rise and fall rate, <strong>the</strong> greater <strong>the</strong> bandwidth<br />

of <strong>the</strong> fiber transport.<br />

Three types of light wavelengths are used <strong>to</strong> transmit signals: short, long, and very<br />

long. Short wavelength light has a wavelength size between 770 and 910<br />

nanometers. Short wavelength light is usually generated by a<br />

gallium-aluminum-arsenide infrared laser or LED with nominal yield of 850<br />

nanometers. Long wavelength light ranges between 1,270 and 1,355 nanometers.<br />

Very long wavelength light ranges between 1,355 and 1,500 nanometers. Both long<br />

and very long wavelength light sources are generated with gallium-indium<br />

arsenide-phosphate infrared lasers. Short and long wavelength light is used for LAN<br />

transmission applications. Very long wavelength light, 1,500 nanometers, is used<br />

exclusively for telecommunications signaling applications such as Synchronous<br />

Optical Network (SONET).<br />

As it passes through <strong>the</strong> fiber strand, <strong>the</strong> light slowly spreads out, and this<br />

phenomenon is known as dispersion. Three forms of dispersion are present in fiber<br />

transport: modal, chromatic, and material. The dispersion fac<strong>to</strong>r determines how<br />

far <strong>the</strong> data can travel across <strong>the</strong> fiber path before <strong>the</strong> signal will be unusable (<strong>the</strong><br />

signal can be repeated or amplified if <strong>the</strong> cable length exceeds <strong>the</strong> dispersion fac<strong>to</strong>r).<br />

Fiber optic cable comes in multimode and single mode. Two differences between<br />

multimode and single-mode fiber are core size and how <strong>the</strong> light travels across <strong>the</strong><br />

core.<br />

The TIA/EIA describes cable using two measurements: <strong>the</strong> core size and <strong>the</strong><br />

cladding size. The TIA/EIA defines two types of multimode fiber: 62.5/125 micron<br />

and 50/125 micron. 62.5/125 micron is <strong>the</strong> standard used by FDDI, 10Base-FL,<br />

100Base-FX, and 1000Base-SX/LX. 50/125 micron is used (and preferred over<br />

62.5/125 micron) only with 1000Base-SX and 1000Base-LX. Single-mode fiber has<br />

a much smaller core size. The TIA/EIA defines <strong>the</strong> single-mode fiber standard as<br />

10/125 microns. With multimode fiber, <strong>the</strong> light bounces off <strong>the</strong> cladding in a rise<br />

and fall pattern across <strong>the</strong> fiber core. With single-mode fiber, <strong>the</strong> light travels<br />

directly through <strong>the</strong> core, as a single beam.

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