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Steel Designers Manual - TheBestFriend.org

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This material is copyright - all rights reserved. Reproduced under licence from The <strong>Steel</strong> Construction Institute on 12/2/2007<br />

To buy a hardcopy version of this document call 01344 872775 or go to http://shop.steelbiz.<strong>org</strong>/<br />

<strong>Steel</strong> <strong>Designers</strong>' <strong>Manual</strong> - 6th Edition (2003)<br />

228 Applied metallurgy of steel<br />

boundary structure. The lattice crystal structure of the ferrite material which forms<br />

the basic matrix is essentially a body-centred cubic structure. Thus in cooling from<br />

the liquid condition, complex changes in both lattice crystal structure and<br />

microstructure take place dependent on the chemical composition. For the equilibrium<br />

diagram conditions to be observed, cooling must be sufficiently slow to allow<br />

time for the transformations in crystal structure and for the diffusion/migration of<br />

carbon to take place to form the appropriate microstructures.<br />

If a steel is cooled from a high temperature and held at a lower constant temperature<br />

for sufficient time, different conditions may result; these are represented<br />

on a diagram known as the isothermal transformation diagram. The form of the<br />

diagram depends on the chemical analysis and in particular on the carbon or related<br />

element content. In plain carbon steels the isothermal transformation diagram typically<br />

has the shape of two letters C each with a horizontal bottom line as shown in<br />

Fig. 6.4. The left-hand/upper curve on the diagram of temperature against time represents<br />

the start of transformation, and the right-hand/lower curve represents the<br />

800<br />

700<br />

600<br />

:::<br />

300<br />

200<br />

100<br />

0 1 10<br />

— — _feit+ pearlite<br />

time (s)<br />

bainite<br />

Fig. 6.4 Isothermal transformation diagram for 0.2% C, 0.9% Mn steel<br />

•stort<br />

106

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