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324 F<strong>org</strong>ing - Sfamping - Heaf Treating<br />
takes place, and very fine grains are temporarily produced.<br />
But grain growth proceeds rapidly at this high<br />
temperature. When the Gamma iron is cooled through<br />
Arl, a good deal of heat is evolved. This tends to retard<br />
cooling and allows time for the grains of Alpha<br />
iron to grow. It is therefore difficult or impossible to<br />
produce a very fine grain size in pure iron, even by<br />
severe quenching.<br />
Anything which will lower the Ar3 transformation<br />
of iron, hinders grain growth. This produces a finer<br />
grained Alpha iron, which is consequently harder and<br />
stronger. Xickel has this effect, and so does carbon.<br />
When carbon (or cementite) goes unto solution in<br />
austenite, it probably does so as atoms of carbon, distributed<br />
among the atoms of iron. The tendency for<br />
the carbon to distribute itself uniformly through the<br />
austenite will cause the carbon atoms to take positions<br />
as far from each other as possible.<br />
When the change from Gamma iron to Alpha iron<br />
takes place, there is a strong tendency for the carbon<br />
to be rejected from solution. In so doing it will combine<br />
with atoms of iron, forming the carbide Fe3C.<br />
"The change from Gamma iron to Alpha iron involves<br />
only minor movements of the iron atoms (face<br />
centered to body centered pattern). Formation of<br />
cementite from iron atoms and carbon atoms, the latter<br />
being as far apart as the}- can get in the space<br />
lattice, involves the diffusion of carbon. This requires<br />
much more time than that required for the<br />
transformation of iron from one space lattice to another."<br />
For this reason the carbon may not be precipitated<br />
when Gamma iron is changed to Alpha iron<br />
by rapid cooling, but may be trapped in the form of<br />
carbon atoms, distributed through the crystalline<br />
grains of Alpha iron.<br />
When austenite, high in carbon, is rapidly cooled,<br />
as by quenching in water, the transformation from<br />
Gamma to Alpha iron is lowered to about 300 deg. C.<br />
Little or no grain growth would occur at this temperature.<br />
The Alpha iron grains are therefore probably<br />
extremely small.<br />
Martensite.<br />
Jeffries and Archer consider martensite, the hardest<br />
state of steel, to be the product of such a quenching<br />
operation and to consist of extremely fine grains of<br />
ferrite in which the carbon is temporarily held as individual<br />
atoms (atomic dispersion).<br />
"Martensite has a variable carbon content, being<br />
the same as that of the austenite from which it was<br />
formed at the moment of the allotropic transformation<br />
(change from Gamma to Alpha iron). Its properties<br />
vary with the carbon content, and with physical differences,<br />
such as those due to different quenching temperature,<br />
or maximum temperature of treatment, before<br />
quenching. Carbon steels containing less than<br />
about 0.15 per cent carbon, do not form hard martensite,<br />
when quenched from above the upper critical temperature.<br />
Carbon steels containing about 0.20 per<br />
cent carbon, form a medium hard but ductile martensite.<br />
The hardness increases with the carbon content<br />
up to about 0.70 per cent carbon, above which there is<br />
a less marked change, up to about 1.50 per cent carbon.<br />
The lower the carbon content, the more drastic<br />
must be the quench, in order to produce martensite.<br />
For example the mildest quench which will produce<br />
100 per cent martensite in a 0.90 per cent carbon steel,<br />
will produce free ferrite, martensite and troostite (or<br />
September, 1925<br />
sorbite) in a 0.20 per cent carbon steel, and martensite<br />
and troostite in a 0.50 per cent carbon steel."<br />
Microstructure of Martensite.<br />
The ferrite grains in martensite probably form<br />
along the cleavage planes of austenite when the latter<br />
is breaking down, and consist of very small thin plates.<br />
This would account for the needle-like appearance of<br />
martensite, and for the peculiar triangular arrangement<br />
of the needles*. (See Figs. 57 and 58, Chapter<br />
III.)<br />
Martensite inherits its appearance, to a still further<br />
extent, from the austenite grains from which it was<br />
formed. If these were large, due to overheating, the<br />
martensite may appear to have distinct grain boundaries,<br />
which, in reality, are merely traces of the austenite<br />
grain boundaries. The larger the parent grains of<br />
austenite, the more pronounced is the needle-like appearance<br />
of martensite. Martensite formed from fine<br />
grained austenite (i.e., which has not been overheated),<br />
has a much less pronounced needle-like structure.<br />
Tempering Martensite.<br />
Since carbon is very much less soluble in Alpha<br />
iron than in Gamma iron, there is a strong tendency<br />
for the entrapped carbon in martensite to precipitate<br />
out, with the formation of carbide. This actually occurs,<br />
when martensite is heated to moderate temperatures,<br />
or even when it is allowed to stand for a time<br />
at room temperature. The cementite so formed gathers<br />
into very minute, submicroscopic particles. As<br />
the temperature is raised, these particles grow in -size,<br />
by the migration of carbon atoms from neighboring<br />
points, and the structure changes to that known as<br />
troostite. A higher temperature results in the forma*<br />
tion of still larger carbide particles, producing the<br />
structure called sorbite. If the tempering temperature<br />
is carried still higher (but below Al), and is held for<br />
a long enough time, relatively large particles are<br />
formed, and we have the structure known as spheroidized<br />
carbide or globular cementite, or sometimes<br />
granular pearlite.<br />
During the first stage of tempering martensite,<br />
perhaps on standing at room temperature, the carbide<br />
particles will grow to the critical size at which they<br />
exert the maximum interference with slip in the ferrite<br />
grains. There is an increase in the hardness of<br />
the martensite up to this point, and it here attains its<br />
maximum hardness. Further increase in the size of<br />
the cabride particles is accompanied by a decrease in<br />
their number, and by a decrease in their effectiveness<br />
as key particles to resist slip. Progressive tempering,<br />
with the formation of troostite, sorbite and globular<br />
cementite therefore reduces the hardness of the steel.<br />
Causes of Hardness of Martensite.<br />
Jeffries and Archer conclude that the hardness of<br />
martensite is due chiefly to the fineness of the ferrite<br />
grains and consider that the presence of great numbers<br />
of minute crystalline particles of cementite, which act<br />
as keys, is an additional source of hardness. Rosenhain<br />
suggests that the presence of insoluble carbon<br />
atoms or the particles of rejected cementite, distorts<br />
•Some microscopic work recently done by Lucas at very hi<br />
magnifications, throws new light on the structure of martensite,<br />
and appears to support the view that it consists of extremely<br />
small plates following the cleavage planes of the parent austenite<br />
grain. See "The Microstructure of Austenite and Martensite "—<br />
F. F. Lucas, Trans. A. S. S. T., Dec, 1924, vol. VI, No. 6.