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Below the important part of the Fe - C
phase diagram is shown. Three lines indicate hypoeutectic, eutectic and
hyereutectic compositions. |
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If we look at what we will find at the indicated
points, this is what we would expect: |
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In all three cases we start with some
polycrystalline g- structure: It is drawn
identically in each cases to point out that the basic phenomena are the same
(and to save work). |
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For the blue hypoeutectic case, we start to grow some a phase as soon as we cross the boundary between the
pure g region and the a + g mixed phase. |
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It is pretty safe to assume that nucleation of the a grains starts at the grain boundaries, in particular
at the nodes. |
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At the eutectic temperature, the a grains have their maximal size. As soon as we cross
over to the a + Fe3C eutectic, the
pure g grains must now transform to a + Fe3C, i.e. to perlite. |
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For the red hypereutectic case, pretty much the same thing
happens |
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We start to grow some Fe3C, i.e. cementite,
as soon as we cross the boundary between the pure g region and the a +
Fe3C mixed phase. |
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It is pretty safe to assume that nucleation of the
Fe3C grains starts at the grain boundaries, but it also sage
to assume that it will be somehow different from the way the a grains did it. This is indicate schematically; we
simply have growth along the boundaries |
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How nucleation and growth takes place in reality, however,
cannot be told from the phase diagram alone; we need some additional
information |
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At the eutectic temperature, the cementite grains have their
maximal size. As soon as we cross over to the a +
Fe3C eutectic, the pure g
grains must now transform to a +
Fe3C, i.e. to perlite. |
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It only remains to discuss what happens if we have
the precise eutectoid composition; this is shown in green. |
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It is simple enough. below the eutectoid temperature, the the
pure g grains transform to a + Fe3C, i.e. to (pure) perlite. |
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However, this does not happen everywhere all at once, again,
some nucleation and growth takes place as indicates. |
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One important point becomes clear, no matter
exactly what happens: The original grain structure of the g phase e very much what kind of grain structure we
will have in the room temperature structure. |
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© H. Föll