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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

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