Fundamentals of Materials Science and Engineering: An Integrated Approach, 3e

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GTBL042-19 GTBL042-Callister-v2 September 13, 2007 13:59


Revised Pages

Summary • 785

Intensity

Ti m e
(a) (b) (c) (d)

Intensity

Ti m e
(e)

Cladding
Core

Radial position
Index of
refraction

Output
impulse

Input
impulse

Figure 19.22 Graded-index optical fiber design. (a) Fiber cross section. (b) Fiber radial
index of refraction profile. (c) Input light pulse. (d) Internal reflection of a light ray.
(e) Output light pulse. (Adapted from S. R. Nagel,IEEE Communications Magazine,
Vol. 25, No. 4, p. 34, 1987.)

periphery of the core travel faster in this lower-index material, and arrive at the out-
put at approximately the same time as undeviated rays that pass through the center
portion of the core.
Exceptionally pure and high-quality fibers are fabricated using advanced and
sophisticated processing techniques, which will not be discussed here. Impurities
and other defects that absorb, scatter, and thus attenuate the light beam must be
eliminated. The presence of copper, iron, and vanadium is especially detrimental;
their concentrations are reduced to on the order of several parts per billion. Like-
wise, water and hydroxyl contaminant contents are extremely low. Uniformity of
fiber cross-sectional dimensions and core roundness are critical; tolerances of these
parameters to within a micrometer over 1 km (0.6 mile) of length are possible. In
addition, bubbles within the glass and surface defects have been virtually eliminated.
The attenuation of light in this glass material is imperceptibly small. For example,
the power loss through a 16-kilometer (10-mile) thickness of optical fiber glass is
equivalent to the power loss through a 25-millimeter (1-inch) thickness of ordinary
window glass!

SUMMARY


Electromagnetic Radiation
Light Interactions with Solids
The optical behavior of a solid material is a function of its interactions with elec-
tromagnetic radiation having wavelengths within the visible region of the spectrum.
Possible interactive phenomena include refraction, reflection, absorption, and trans-
mission of incident light.

Optical Properties of Metals
Metals appear opaque as a result of the absorption and then reemission of light
radiation within a thin outer surface layer. Absorption occurs via the excitation of
electrons from occupied energy states to unoccupied ones above the Fermi energy
level. Reemission takes place by decay electron transitions in the reverse direction.
The perceived color of a metal is determined by the spectral composition of the
reflected light.
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