26.03.2017 Views

Materials for engineering, 3rd Edition - (Malestrom)

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Structure of <strong>engineering</strong> materials 15<br />

of a two-dimensional plot of temperature versus composition, which marks<br />

out the composition limits of the phases as functions of the temperature. We<br />

will now introduce some simple examples of phase diagrams, which we will<br />

correlate with some microstructures.<br />

Solid solubility<br />

In a solid solution, the crystal structure is the same as that of the parent<br />

element – the atoms of the solute element are distributed throughout each<br />

crystal and a range of composition is possible. The solution may be <strong>for</strong>med<br />

in two ways:<br />

(a) in interstitial solid solutions, the atoms of the solute element are small<br />

enough to fit into the spaces between the parent material atoms, as<br />

illustrated in Fig. 1.10(a). Because of the atom size limitation involved,<br />

interstitial solid solutions are not common, although, in steel, carbon<br />

atoms dissolve to a limited extent in iron crystals in this way.<br />

(b) in substitutional solid solutions, the atoms share a single common array<br />

of atomic sites as illustrated in Fig. 1.10(b). Zinc atoms may dissolve in<br />

this way in a copper crystal (up to approximately 35% zinc) to <strong>for</strong>m brass.<br />

A few pairs of metals are completely miscible in the solid state and are<br />

said to <strong>for</strong>m a ‘continuous solid solution’; copper and nickel behave in this<br />

way and the phase diagram <strong>for</strong> this system is shown in Fig. 1.11. The horizontal<br />

scale shows the variation in composition in weight per cent nickel and the<br />

vertical scale is the temperature in °C. The diagram is divided into three<br />

‘phase fields’ by two lines – the upper phase boundary line is known as the<br />

liquidus and the lower line as the solidus. At temperatures above the liquidus,<br />

alloys of all compositions from pure copper to pure nickel will be liquid,<br />

while at temperatures below the solidus, all alloys are in the solid state. It<br />

will be apparent that, unlike pure metals, alloys freeze over a range of<br />

temperature whose magnitude depends upon the composition of the alloy<br />

(a)<br />

1.10 Solid solutions <strong>for</strong>med (a) interstitially and (b) substitutionally.<br />

(b)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!