FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
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