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Natural Science in Archaeology

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36 2 Properties of M<strong>in</strong>erals<br />

m<strong>in</strong>erals. Sphalerite, ZnS, is colorless when pure and assumes its typical honeybrown<br />

color when iron substitutes for z<strong>in</strong>c <strong>in</strong> the structure. Willemite, Zn 2 SiO 4 ,<br />

is also colorless when pure but develops a variety of colors through chemical<br />

substitution of other elements <strong>in</strong> the structure. The follow<strong>in</strong>g transition elements<br />

produce the color <strong>in</strong>dicated <strong>in</strong> parentheses when <strong>in</strong>troduced <strong>in</strong>to willemite: copper<br />

(light green), iron (gray), manganese (yellow), chromium (gray), and cobalt<br />

(<strong>in</strong>tense blue).<br />

It is often difficult to determ<strong>in</strong>e completely the cause of color when transition<br />

metals are present, because effects aris<strong>in</strong>g from partially filled d orbitals may be<br />

masked by the strong absorb<strong>in</strong>g power of charge-transfer phenomena also common<br />

<strong>in</strong> m<strong>in</strong>erals conta<strong>in</strong><strong>in</strong>g transition metals.<br />

The Effects of Chemical Bond<strong>in</strong>g. “Free” electrons give metals their characteristic<br />

opacity (by absorption), their high reflect<strong>in</strong>g power (“metallic” luster), and, <strong>in</strong><br />

many cases, their color. Two dist<strong>in</strong>ct mechanisms, both dependent on the different<br />

manner <strong>in</strong> which the electrons <strong>in</strong> metals respond to different parts of the visible<br />

spectrum, are important <strong>in</strong> def<strong>in</strong><strong>in</strong>g the optical properties of metals. One is selective<br />

reflection, and the other is selective absorption. Selective reflection may be<br />

the dom<strong>in</strong>ant mechanism <strong>in</strong> highly reflect<strong>in</strong>g m<strong>in</strong>erals such as metals. Gold exhibits<br />

a yellow color due to selective reflection of yellow light, not selective absorption.<br />

Light transmitted through th<strong>in</strong> gold foil is bluish green; the yellow has been<br />

reflected and the red absorbed.<br />

F<strong>in</strong>ely powdered metals show a strong general absorption and appear black due<br />

to the large number of small light traps between the particles. Light is cont<strong>in</strong>ually<br />

reflected back and forth among the small metal gra<strong>in</strong>s. On each contact with a metal<br />

surface a little more light is absorbed, ultimately result<strong>in</strong>g <strong>in</strong> total absorption and<br />

ext<strong>in</strong>ction of the light.<br />

The color absorption characteristics of covalently bonded m<strong>in</strong>erals depend on<br />

how tightly the bond<strong>in</strong>g electrons are held <strong>in</strong> the elements. In diamond these electrons<br />

are held securely, result<strong>in</strong>g <strong>in</strong> electromagnetic wave absorption only <strong>in</strong> the<br />

ultraviolet region; therefore, a diamond crystal appears colorless and transparent.<br />

In silicon the electrons are not as tightly held, so absorption occurs <strong>in</strong> the visible<br />

spectrum, and the material is colored or opaque. T<strong>in</strong> has the same crystal structure<br />

as diamond and silicon, but the electrons are so loosely held that pure t<strong>in</strong> is opaque<br />

and has properties we normally associate with metals, although it is not a true<br />

metal.<br />

The element carbon illustrates well the color variations due to different bond<br />

strengths <strong>in</strong> the same element. In diamond the strong bond<strong>in</strong>g results <strong>in</strong> a dense,<br />

very hard m<strong>in</strong>eral that is transparent and colorless. The m<strong>in</strong>eral graphite, however,<br />

is also composed solely of carbon. Here a different type of bond<strong>in</strong>g produces a large<br />

number of loosely bonded electrons that absorb almost the entire visible spectrum,<br />

result<strong>in</strong>g <strong>in</strong> a deep black opaque m<strong>in</strong>eral (Fig. 2.9).<br />

Pure quartz, SiO 2 , is transparent and colorless. Crystals of quartz are transparent<br />

to wavelengths of electromagnetic radiation rang<strong>in</strong>g all the way from 1800<br />

to 300,000 angstrom units. However, s<strong>in</strong>ce impurities are often <strong>in</strong>cluded <strong>in</strong> the<br />

crystal, colored varieties of quartz are common. Some amethyst<strong>in</strong>e quartz owes its

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