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July, 1925<br />
Solubility.<br />
Gamma iron (austenite), is able to hold moderate<br />
quantities of carbon in solid solution. The presence<br />
of dissolved carbon lowers the temperature at which<br />
Gamma begins to change to Alpha iron on cooling.<br />
This causes a downward slope of the line GS, representing<br />
A3 (and A2, 3), in the diagram, from 900 deg.<br />
C. for pure iron, to 725 deg. C. for iron containing 0.90<br />
per cent carbon*.<br />
Alpha iron (ferrite), is able to hold in solid solution<br />
considerable quantities of certain elements, such as<br />
nickel, silicon and phosphorus, but very little carbon.<br />
The maximum amount of carbon it can take up, is<br />
probably about 0.05 per cent to 0.10 per cent. This<br />
fact has an important bearing on the hardening of steel,<br />
as will be shown.<br />
Hypo-Eutectoid Steel.<br />
Let us now consider a hypo-eutectoid steel, containing,<br />
say, 0.30 per cent carbon, which is heated to a<br />
temperature above A3. It will consist entirely of austenite—that<br />
is, grains of Gara_ma iron holding the carbon<br />
in solid solution. If the piece is allowed to cool<br />
slowly, to the Ar3 point, some of the austenite (Gamma<br />
iron) will change to ferrite, which will separate as<br />
a distinct constituent which we may call "free ferrite."<br />
Since this ferrite is unable to hold appreciable amounts<br />
of carbon in solid solution, the carbon which was in<br />
it will go into solution in the remaining austenite.<br />
This will increase the carbon content of the austenite<br />
and will therefore lower the temperature at which<br />
ferrite separates out. As cooling continues, more ferrite<br />
will be liberated, and the remaining austenite will<br />
become richer in carbon. The diminishing austenite<br />
must hold all of the carbon which is present in the<br />
steel. When a temperature of 725 deg. C. has been<br />
reached, the specimen will consist of two-thirds ferrite,<br />
containing practically no carbon, and one-third<br />
austenite, containing 0.90 per cent carbon. At this<br />
temperature, which is the point Al, austenite will<br />
take no more carbon into solution—it is saturated.<br />
Further slow cooling will now cause the austenite<br />
to break down into ferrite and cementite (Fe3C).<br />
These two constituents will separate in alternate thin<br />
plates or lamellae, producing what we know as pearlite.<br />
Each grain of austenite which remained at 825<br />
deg. C, is converted bodily into one or more grains of<br />
pearlite. These pearlite grains will be imbedded in<br />
or>surrounded by, free ferrite.<br />
No change takes place in the free ferrite on cooling<br />
thru the Al point. This point is caused by the conversion<br />
of the austenite into pearlite, and its intensity<br />
therefore increases from zero, in carbonless iron, up<br />
to a maximum in steel containing 0.90 per cent carbon.<br />
The intensity of the point depends upon the<br />
amount of austenite present at the Al temperature.<br />
F<strong>org</strong>ing- Stamping - Heat Treating<br />
*There is some question whether the line GOS should run<br />
straight from the point G to the point S, on the iron-carbon diagram,<br />
or whether it should be curved or bend downward to the<br />
Point O. Critical point diagrams, used in connection with heattreating<br />
practice, almost always show the latter construction.<br />
This seems to be justified by actual experience. Archer, in ref.<br />
12, makes the line straight, because he considers that there is insufficient<br />
evidence upon which to base the construction of a<br />
curved or broken line. In Fig. 110 the usual practice in the construction<br />
of critical point diagrams has been followed, and the<br />
line has been shown broken at O. The curves of Carpenter and<br />
Keeling, Sauveur, Fig. 175, ref. 8, are substantially in agreement<br />
with this construction.<br />
245<br />
The ferrite which separa-ted from the solid solution<br />
above the A2 point (768 deg. C), was in the nonmagnetic<br />
or Beta state. Upon cooling through Ar2,<br />
this ferrite changed to magnetic or Alpha ferrite (without<br />
any change in its crystalline structure). Further<br />
separations of ferrite with falling temperature, were<br />
in the Alpha state.<br />
Suppose that we now have a specimen of hypoeutectoid<br />
steel containing 0.60 per cent carbon, heated<br />
to the austenitic state, that is, above A2, 3. This<br />
specimen will cool to about 750 deg. C. before separation<br />
of ferrite begins. Separation of carbonless ferrite<br />
in the Alpha state, will continue down to the Al point<br />
(725 deg. C). The steel will then consist of one-third<br />
ferrite and two-thirds austenite, the latter containing<br />
all of the carbon and having a carbon content of 0.90<br />
per cent. Upon cooling through Arl, the grains of<br />
austenite will be converted into grains of pearlite.<br />
It may be that in separating from austenite at temperatures<br />
below 768 deg. C, the ferrite first takes<br />
the Beta form, and then immediately changes to the<br />
Alpha form. On the other hand, Gamma iron may<br />
change directly into Alpha iron when the A3 point is<br />
below 768 deg. C. In either case, there will be a<br />
change from a non-magnetic to a magnetic state on<br />
cooling, and we may regard the A2 point as following<br />
the line OSK in the diagram.<br />
A<br />
? v<br />
*+<br />
i m<br />
j £ S<br />
m<br />
w<br />
FIG. Ill (left)—Alpha iron, body centered cubic arrangement.<br />
FIG. 112 (right)—Gamma iron, face centered cubic arrangement.<br />
(Archer.)<br />
Eutectoid Steel.<br />
Let us now consider a specimen containing 0.90<br />
per cent carbon (the eutectoid composition). When<br />
heated above the critical temperature, this piece will<br />
consist of austenite, holding 0.90 per cent carbon in<br />
solid solution. No change will take place on cooling,<br />
until the Al point (725 deg. C), is reached. Here<br />
the entire mass will be converted into pearlite. At<br />
the same-time, the steel will change from the non-magnetic<br />
to the magnetic state.<br />
Hyper-Eutectoid.<br />
Suppose now that we have a hyper-eutectoid steel<br />
containing say, 1.20 per cent carbon, heated above the<br />
Acm point (for example to 900 or 950 deg. C). All<br />
of the carbon will be held in solid solution in the<br />
austenite. But the solubility of carbon in austenite<br />
decreases as the temperature is lowered, and upon cooling<br />
to the Acm point (the line Se), excess carbon in<br />
the form of cementite will begin to precipitate from<br />
the solid solution. More cementite will-be precipitated<br />
as cooling continues. This will lower the carbon content<br />
of the austenite, until, when a temperature of 725<br />
deg. C. is reached, the austenite will have only 0.90<br />
per cent carbon in solution. The remaining carbon<br />
will be present in the form of free cementite, Fe3C.<br />
The Al change will now take place, that is, the grains<br />
7