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Materials for engineering, 3rd Edition - (Malestrom)

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1<br />

Structure of <strong>engineering</strong> materials<br />

1.1 Crystal structure<br />

Crystal structure refers to the ordering of atoms into different crystalline<br />

arrangements. It is the arrangement of these atoms – the strength and<br />

directionality of the interatomic bonds – which determines the ultimate strength<br />

of the solid. Techniques involving X-ray or electron diffraction are employed<br />

to determine crystal structures, and four types of interatomic bonding are<br />

recognized: van der Waals, covalent, ionic and metallic. The latter three<br />

‘primary’ bonds are limiting cases, however, and a whole range of intermediate<br />

bonding situations also exist in solids.<br />

The van der Waals <strong>for</strong>ce is a weak ‘secondary’ bond and it arises as a<br />

result of fluctuating charges in an atom. There will be additional <strong>for</strong>ces if<br />

atoms or molecules have permanent dipoles as a result of the arrangement of<br />

charge inside them. In spite of their low strength, these <strong>for</strong>ces can still be<br />

important in some solids; <strong>for</strong> example it is an important factor in determining<br />

the structure of many polymeric solids.<br />

Many common polymers consist of long molecular carbon chains with<br />

strong bonds joining the atoms in the chain, but with the relatively weak van<br />

der Waals bonds joining the chains to each other. Polymers with this structure<br />

are thermoplastic, i.e. they soften with increasing temperatures and are readily<br />

de<strong>for</strong>med, but on cooling they assume their original low-temperature properties<br />

and retain the shape into which they were <strong>for</strong>med.<br />

Covalent bonding is most simply exemplified by the molecules of the<br />

non-metallic elements hydrogen, carbon, nitrogen, oxygen and fluorine. The<br />

essential feature of a covalent bond is the sharing of electrons between<br />

atoms, enabling them to attain the stable configuration corresponding to a<br />

filled outermost electron shell. Thus, an atom with n electrons in that shell<br />

can bond with only 8 – n neighbours by sharing electrons with them.<br />

For example, when n = 4, as in carbon in the <strong>for</strong>m of diamond, one of the<br />

hardest materials known, each atom is bonded equally to four neighbours at<br />

the corners of a regular tetrahedron and the crystal consists of a covalent<br />

3

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