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FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

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v<br />

vacancy defect. In the somewhat ordered array of atoms<br />

and molecules in optical-fiber material, a site at<br />

which an atom or molecule is missing in the array.<br />

The defect can serve as a scattering center, causing<br />

diffusion, heating, absorption and resultant attenuation.<br />

Also see interstitial defect.<br />

valence band. In a semiconductor, the range of electron<br />

energy, lower than that of the conduction<br />

band, possessed by electrons that are held bound to<br />

an atom of the material, thus reducing conductivity<br />

for electric currents even under the influence of<br />

an applied electric field. When electron engergies<br />

are raised, e.g., by thermal excitation or by phonons,<br />

electrons with the highest energy levels of<br />

the valence band are raised to the lower energy<br />

levels of the conduction band, thus leaving holes<br />

in the atoms whose electrons remain in the valence<br />

band.<br />

velocity.<br />

See phase velocity.<br />

V-parameter. A parameter that can be used to calculate<br />

or express the number of propagating modes that a<br />

step-indexed optical fiber is capable of supporting,<br />

expressed mathematically as:<br />

fn =<br />

(2na/k)(n12 - n22)1/2<br />

where fn is the V-parameter (V-value or normalized<br />

frequency), a is the optical fiber core radius, Ais<br />

the source wavelength, and nl and n2 are the refractive<br />

indices of the core and cladding of the optical<br />

fiber. For a large number of modes, the mode volume<br />

is given by:<br />

N = fn2/2<br />

where N is the number of modes, or mode volume, and<br />

fn Is the V-parameter (V-value or normalized frequency)<br />

above. Synonymous with normalized frequency;<br />

V-value.<br />

V-value. Synonym for V-parameter.<br />

wave.<br />

w<br />

See electromagnetic wave; evanescent wave.<br />

wave equation. The equation, based on Maxwell’s equations,<br />

the constitutive relations, and the vector<br />

algebra, that relates the electromagnetic field of<br />

an electromagnetic wave time and space derivatives<br />

with the transmission medium electrical permittivity<br />

and magnetic permeability in a region without electrical<br />

charges or currents. The solution of the wave<br />

equation yields the electric and magnetic field<br />

strength everywhere as a function of time and space<br />

coordinates, field strengths, and transmission media<br />

parameters. The wave equation is given as either:<br />

72H- ~ca2H/at2 = o ‘r<br />

v2E - vEa2E/at2 = o<br />

in a current- and charge-free nonconducting medium,<br />

where E is the electric field intensity, H is the<br />

magnetic field intensity, c is the electric permittivity,<br />

and p is the magnetic permeability. V is the<br />

vector spatial derivative operator. The wave equation<br />

applies in optical waveguides.<br />

wavefront. A surface normal to an electromagnetic ray<br />

as it propagates from a source, the surface of the<br />

wavefront passing through those parts of the waves<br />

that are in the same phase. For parallel rays, the<br />

wavefront is a plane. For rays diverging from or<br />

converging toward a point, the wavefront is spherical.<br />

The wavefront is perpendicular to the direction<br />

of propagation of the wave, and the electric<br />

and magnetic field vectors of the wave define a<br />

plane that is tangent to the wavefront surface at<br />

the point that the field vectors are determined.<br />

The front is a three-dimensional surface all the<br />

points on which are the same optical path length<br />

from the wave source.<br />

waveguide. Any structure capable of confining and supporting<br />

the energy of an electromagnetic wave to a<br />

specific relatively narrow controllable path that is<br />

capable of being altered, such as a rectangular<br />

cross-section metal pipe, an optical fiber of circular<br />

cross section, or a coaxial cable. See slab<br />

dielectric waveguide.<br />

waveguide delay distortion. In an optical waveguide,<br />

the distortion in received signal caused by the differences<br />

in propagation time for each wavelength,<br />

(i.e., the delay versus wavelength effect for each<br />

propagating mode), causing a spreading of a received<br />

signal pulse at the detector. Waveguide delay distortion<br />

contributes to group-delay distortion as<br />

does material dispersion and multimode group-delay<br />

spread.<br />

waveguide dispersion. The part of the total dispersion<br />

attributable to the dimensions of the waveguide. The<br />

cross-section dimensions are critical. They determine<br />

the modes that are allowed and not allowed to<br />

propagate. Waveguide dispersion increases as the<br />

spectral width of the source increases due to the<br />

actual dimensions and their variation along the<br />

length of the guide.<br />

wavelength. The length of a wave measured from any<br />

point on a wave to the corresponding point on the<br />

next cycle of the wave, such as from crest to crest.<br />

Wavelength determines the nature of the various<br />

forms of radiant energy that comprise the electromagnetic<br />

spectrum, e.g., it determines the color of<br />

light. For a sinusoidal wave, the wavelength is the<br />

distance between points of corresponding phase of<br />

two consecutive cycles of the wave. The wavelength<br />

k, iS related to the phase velocity v, and the frequency<br />

f, by the relation i= vlf.<br />

wavelength-division multiplexingg (WDM). In optical communication<br />

systems, the multiplexing of lightwaves in<br />

a single transmission medium or channel, such that<br />

each of the waves are of a different wavelength and<br />

are modulated separately before insertion into the<br />

medium. Usually, several sources are used, such as<br />

a laser, or several lasera, or a dispersed white<br />

light source or aources, each having a distinctly<br />

different center wavelength. WDM is the same as<br />

frequency-division multiplexing (FDM) applied to<br />

visible light frequencies of the electromagnetic<br />

spectrum.<br />

wave number. The value of 2n times the reciprocal of<br />

the wavelength of a single-frequency sinusoidal wave<br />

such as a singlefrequency uniform plane-polarized<br />

A-22

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