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September, 1925<br />
the space lattice of the ferrite grains, thereby interfering<br />
with slip. He believes that this is an important<br />
cause of hardness.<br />
Formation of Troostite and Sorbite on Quenching.<br />
We have seen in Chapter III that martensite is not<br />
always formed on quenching, but that slower cooling,<br />
or lower carbon content will produce the softer constituents,<br />
troostite and sorbite. Slower cooling and<br />
less carbon does not lower the transformation point so<br />
much as rapid cooling and high carbon. A higher temperature<br />
and longer time favor the formation of larger<br />
grains of Alpha iron, and the precipitation and growth<br />
of cementite particles. There is therefore less resistance<br />
to slip, and consequently less hardness, than in<br />
martensite.<br />
Migration of Carbon in Alpha Iron.<br />
Below the Al point, iron (that is, Alpha iron or<br />
ferrite), will dissolve very little carbon. The amount<br />
it will retain in solid solution after slow cooling from<br />
above the critical point, is certainly less than about .05<br />
per cent, as is evident from the fact that steel containing<br />
this much carbon will show islands of pearlite after<br />
annealing. It is therefore usually said that cementite<br />
or carbon is insoluble in Alpha iron. This, however,<br />
cannot be strictly true. Troostite is known to consist<br />
of Alpha iron in which are embedded innumerable<br />
crystalline particles of cementite, too small to be seen<br />
FIG. 120—Grain growth by strain. Tapered bar of mild steel,<br />
broken in tension and then heated to about 600 deg. C. for 2<br />
hours. Longitudinal section. Low magnification. (C.<br />
Chappell.)<br />
F<strong>org</strong>ing- Sf amping - Heaf Treating<br />
325<br />
Grain Growth Below Critical Range.<br />
We have seen that grain growth takes place in steel<br />
when it is heated above the critical range, but that,<br />
ordinarily, none occurs below the critical range. There<br />
are exceptions to this rule, which should be noted.<br />
Pronounced grain growth may occur in low carbon<br />
steel (carbon about 0.04 to 0.12 per cent) at temperatures<br />
below the critical range, if it is in a cold worked<br />
state — that is, if strains have been set up in the<br />
metal. For a certain temperature there is a certain<br />
degree of strain that will produce the greatest grain<br />
growth. For instance, if a tapered bar is annealed,<br />
so as to remove all strain and produce a fairly fine<br />
grain structure, then broken in tension and finally<br />
heated to some temperature below the Al point, such<br />
as 600 deg. C, quite large grains may be produced at<br />
some point along its length. Since the bar was tapered,<br />
the stress, and therefore the strain, will have increased<br />
gradually from the thickest part to the thinnest.<br />
The section at which the strain was most favorable<br />
for grain growth at 600 deg. C, will have the largest<br />
grains. Higher and lower strains will have produced<br />
less grain growth. For a different temperature,<br />
maximum grain growth would have occurred at some<br />
other section. The experiment is illustrated in Fig.<br />
120.<br />
A "temperature gradient", that is a condition<br />
wherein the temperature increases from one point to<br />
another, in the piece, may also cause grain growth in<br />
steel.<br />
The reasons for these exceptions to the ordinary<br />
laws of grain growth, are still uncertain. The subject<br />
is discussed at some length in ref. 13.<br />
In view of the pronounced effect of grain size on<br />
the properties of metal the importance of these exceptional<br />
cases of grain growth is plain.<br />
Volume Changes.<br />
When austenite changes to martensite on quench<br />
under the microscope. If troostite is heated to a temping, there is an increase in volume camparable to that<br />
erature slightly below the Al point, say 700 deg. C. which takes place in soft iron on slow cooling through<br />
for several hours, cementite particles large enough to Ar3. This expansion during quenching, takes place<br />
be seen under high magnification, will be formed. The at a temperature below 300 deg. C. It is accompanied<br />
structure will have changed to sorbite. Continued by reappearance of magnetism and the development<br />
heating below the critical range, will cause the cemen of pronounced hardness. If austenite, which has been<br />
tite particles to increase in size, but decrease in num preserved at ordinary temperatures, is caused to<br />
ber, resulting in the structure known as spheroidized<br />
change into martensite, by tempering, a similar ex<br />
cementite or granular pearlite. The particles of cemenpansion<br />
takes place.<br />
tite in troostite or sorbite are not connected, and are When freshly formed martensite is allowed to stand<br />
completely surrounded by ferrite. In order for some at room temperature for a time, or is slightly heated<br />
of them to grow, carbon or carbide from neighboring as by placing in boiling water, contraction takes place.<br />
particles must travel to them through the ferrite. The Tempering causes further contraction. This contrac<br />
large particles grow by taking material from smaller tion is attributed to the formation (precipitation) of<br />
particles, through the intervening ferrite. It is cementite. The individual carbon atoms, entrapped<br />
considered that the small particles gradually dis in Alpha iron during sudden cooling, probably take up<br />
solve in the surrounding ferrite, and that carbon atoms more room than they do when combined with iron<br />
then migrate through the ferrite to the larger particles. atoms in the form of cementite, Fe3C.<br />
combining there with iron atoms to form carbide The amount of contraction which takes place, in<br />
(Fe3C) again, and becoming part of the larger cemencreases with the carbon content. In steel containing<br />
tite particle. This means that the larger particles have 1.0 per cent carbon, the contraction due to the forma<br />
a stronger tendency to grow than do the small partition of cementite is sufficient to counterbalance the<br />
cles. (We have seen that the same principle holds true expansion which accompanies the formation of Alpha<br />
in the crystalline grains of metal, and accounts for iron from Gamma iron. Such steel, when slowly cooled<br />
grain growth.) The cementite particles could not grow through the critical range, undergoes no volume<br />
in this way, unless carbide or carbon is soluble, to change except the gradual contraction due to cooling.<br />
some extent, in ferrite. The solubility is no doubt If it is suddenly cooled, so as to form martensite, ex<br />
greater just below Al than at lower temperatures, and pansion occurs, and this is followed by contraction on<br />
is probably about 0.10 per cent.<br />
standing or on tempering.