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ATTENUATION AND W VELENGTH In high school physics classes, A instructors often talk about relationships between physical parameters In the world of electrical communications, we probably heard the expression high frequencies attenuate more rapidly than low frequencies If we put on our thinking caps and remember that wavelength is inversely proportional to frequency we can express a general relationship , between attenuation and wavelength That general relationship can be expressed as attenuation decreases as the wavelength increases In more technical terms, the dispersion of electromagnetic radiation varies inversely to the fourth power of the wavelength This dispersion or scattering is referred to as Rayleigh scattering, after Lord Rayleigh, who in 1871 published a paper that described this phenomenon.

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Rayleigh scattering explains the blue color of the sunlit sky since blue light, which is locat, ed at the short-wavelength portion of the visible spectrum, will be scattered more strongly than longer wavelengths, such as green, yellow, orange, and red Thus, when we view the sky in a direction other than toward the sun, we observe scattered light, which appears blue Mathematically we can denote the Rayleigh effect as I 1/ 4 As an example of the Rayleigh effect, scattering at 400 nm becomes 94 times as great as that 700 nm when a person views a common location Thus, if we plot attenuation as a function of wavelength and consider the effect of Rayleigh scattering only the relationship would appear as , shown in the top portion of Figure 310.

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If we consider only the Rayleigh effect, we would always want to operate at a relatively long wavelength to minimize attenuation However another important characteristic of light , that we need to consider is its absorption Absorption is caused by residual impurities in the fiber In addition, it is nonlinear with absorption , higher at some wavelengths than others This is shown in the middle portion of Figure 310 In case you are wondering about the bump in the degree of attenuation beginning at 1350 nm, that increase results from the effect of light between 1350 and 1450 nm in the presence of hydroxyl radicals in the cable material In some publications you will note the term OH absorption at the top of the peak at approximately 1400 nm to denote the effect of hydroxyl radicals.

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Thus, the actual attenuation spectrum as a function of wavelength is a complex process When we consider both the Rayleigh effect and absorption, the plot of attenuation versus wavelength appears as shown in the lower portion of Figure 310 If you focus on the vertical bars in the lower portion of.

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