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FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

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N<br />

nanometer. One thousandth of a micron, i.e. , 10-9<br />

met er.<br />

near total internal reflection sensor. In fiberoptic,<br />

a fiberoptic sensor that operates on the principle<br />

of varying the property of an optical fiber in such<br />

a manner that the amount of light that leaks into<br />

the cladding ie altered by varying the critical angle<br />

in accordance with a baseband signal, auch as by<br />

altering the refractive index or the ordinary bend<br />

radius, thus altering the internal reflection.<br />

noise. In a fiberoptic system, the sum of unwanted or<br />

disturbing energy introduced into the system from<br />

natural or man-made sources, such as unwanted lightwaves<br />

coupled into an optical fiber or unwanted modulation<br />

of lightwaves in an optical fiber due to environmental<br />

conditions that alter the propagation or<br />

modulation characteristics of an optical fiber or<br />

fiberoptic sensor.<br />

noise power. The power that is developed by unwanted<br />

electromagnetic waves from all sources in the output<br />

of a device, such as a transmission channel or amplifier.<br />

Noise power is usually the total noise power<br />

of waves with frequencies within the passband of the<br />

system or device. Croastalk, distortion, and lntermodulation<br />

products are usually classed as noise.<br />

normalized frequency.<br />

See V-parameter.<br />

numerical aperture (N.A.). A measure of the light-accepting<br />

property of an optical fiber. For example,<br />

glass; given by:<br />

N.A. = (n12-n22)1/2<br />

i.e., the square root of the difference of the<br />

squares of the refractive indices of the core, nl,<br />

and the cladding, n2. If nl is 1.414 (glass) and n2<br />

is 1.0 (air), the numerical aperture is 1.0 and all<br />

incident rays will be trapped. The numerical aperture<br />

is a measure of the characteristic of an optical<br />

waveguide in terms of its acceptance of impinging<br />

light. The degree of openness, light-gathering<br />

ability, angular acceptance, and acceptance cone are<br />

all terms describing the characteristic. It may be<br />

necesaary to specify that the refractive indices are<br />

for step index fibera and for graded index fibers;<br />

nl is the maximum index in the core and n2 is the<br />

minimum Indexin the cladding. As a number, theN.A.<br />

expresses the Mghtgathering power of a fiber. It<br />

is mathematically equal to the sine of the acceptance<br />

angle. A method of meaauring the N.A. is to excite<br />

the fiber in the visible region and display the light<br />

emerging from the end perpendicularly on a screen<br />

about 10 to 30 cm away. The measured diameter of<br />

the projected circle of light divided by twice the<br />

distance from the fiber end to the screen is the<br />

numerical aperture. The numerical aperture is also<br />

equal to the sine of the half-angle of the widest<br />

bundle of rays capable of entering a lens, multiplied<br />

by the refractive index of the medium containing<br />

that bundle of rays, i.e., the incident medium.<br />

Typical numerical apertures for plastic-clad fused<br />

silica optical fibers range from 0.25 to 0.45.<br />

optic.<br />

optical cable.<br />

See fiberoptic.<br />

optical circuit.<br />

optical data link.<br />

0<br />

See fiberoptic cable.<br />

See integrated optical circuit.<br />

See fiberoptic data link.<br />

optical fiber. A single discrete optical transmission<br />

element or waveguide usually consisting of a fiber<br />

core and a fiber cladding that can guide a lightwave<br />

and is usually cylindrical in shape. It consists<br />

either of a cylinder of transparent dielectric material<br />

of a given refractive index whose walls are in<br />

contact with a second dielectric material of a lower<br />

refractive index; or of a cylinder whose core has a<br />

refractive index that gets progressively lower away<br />

from the center. The length of a fiber is usually<br />

much greater than its diameter. The fiber relies<br />

upon internal reflection to transmit light along its<br />

axial length. Light enters one end of the fiber and<br />

emerges from the opposite end with losses dependent<br />

upon length, absorption, scattering, and other factors.<br />

A lightwave in an optical fiber can be modulated<br />

by changing the light propagation parameters<br />

of the fiber. A bundle of fibers has the ability<br />

to transmit a picture from one of its surfaces to<br />

another, around curves, and into otherwise inaccessible<br />

places with an extremely low losa of definition<br />

and light, by the proceas of total internal reflection.<br />

One optical fiber classification scheme is<br />

to divide them into plastic, glaas, or plastic-clad<br />

fuaed silica fibers; then into step-index multimode,<br />

graded-index multimode, or step-index single mode<br />

fibers. Plastic is less brittle than glass but has<br />

increased attenuation compared to glass. Synonymous<br />

with light pipe. See self-focusing optical fiber.<br />

optical fiber coating. A protective material bonded to<br />

an optical fiber over the cladding to preserve fiber<br />

atrength and inhibit cabling losses by providing protection<br />

againat mechanical damage, protection against<br />

moisture and debilitating environments, compatibility<br />

with fiber and cable manufacture, and compatibility<br />

with the jacketing proceas. Coatings include<br />

fluorpolymers, Teflonc, Kynarc, polyurethane,<br />

and many others. Application methods include dipcoating<br />

(for those in solution), extrusion, spray<br />

coating, and electrostatic coating.<br />

optical fiber jacket. A material used to cover an optical<br />

fiber, whether or not it is cladded or coated.<br />

optical fiber loss. The optical power loss in an optical<br />

fiber, usually expressed in dB/km.<br />

optical fiber preform. Specially-shaped material from<br />

which an optical fiber is made, usually by drawing<br />

or rolling. For example, a solid glass rod made with<br />

a higher refractive index than the tube into which<br />

it is alipped,<br />

into a cladded optical fiber; or<br />

tive-index rods surrounding a<br />

index rod heated and drawn into a<br />

drawing procesa results in fiber<br />

than the preforma.<br />

to be heated and drawn or rolled<br />

four lower-refrachigher-refractivecladded<br />

fiber. The<br />

many times longer<br />

A-14

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