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L-07
             ENGINEERING MATERIALS
    TRANSFORMATIONS ON HEATING COOLING




10/14/2011                           1
Microstructure of Fe-C
                  Martensites
• Martensite commonly is found in
  tools such as hammers, chisels and
  in swords.
• Martensite is a hard, brittle form of
  steel with a tetragonal crystalline
  structure, created by a process
  called martensitic transformation.
• It is named after metallurgist Adolf
  Martens (1850-1914), who
  discovered its structure under his
  microscope during his
  metallographic research and
  explained how the physical
  properties of different types of steel
  were affected by their microscopic
  crystalline structures.

10/17/2011                             2
Structure of Fe-C on an
     atomic scale
  Martensite is made from austenite, a
   solid solution of carbon and iron with a
   face-center cubic crystalline structure
   that is formed by heating iron to a
   temperature of at least 723 degrees C.
  Martensitic transformation occurs when
   the austenite is rapidly cooled in a
   process known as quenching.
  The rapid drop in temperature traps
   carbon atoms inside the crystal
   structures of the iron atoms before they
   can diffuse out, resulting in a slight
   distortion of the shape of these
   structures that greatly increases the
   steel's hardness.
  The resulting martensitic steel is
   extremely hard but very brittle.



10/17/2011                                    3
Structure of Fe-C on an atomic
                 scale
• Thus, the martensite is then
  heated in a process called
  tempering, which causes the
  martensite to transform partially
  into ferrite and cementite. This
  tempered steel sacrifices
  hardness but results in steel that
  is tougher and more malleable
  than pure martensite alone, so it
  is better suited for industrial use.
• For carbon contents in FeC
  martensites of less than about
  0.2%C, the austenite transforms
  to a BCC ferrite crystal
  structure. As the carbon content
  of the FeC alloys is increased, the
  BCC structure is distorted into a
  BCT crystal structure.
10/17/2011                               4
Structure of Fe-C on an
      atomic scale
     The largest interstitial hole in the
     iron FCC crystal structure has a
     diameter of 0.104 nm(Fig 9.17a),
     whereas the largest interstitial hole
     in the iron BCC structure has a
     diameter of 0.072 nm (Fig 9.17b).
     Since the carbon atom has a
     diameter of 0.154nm, it can be
     accommodated in interstitial solid
     solution to a greater extent in the
     FCC iron lattice.



                           FIG 9.17

5                                      10/14/2011
Hardness and strength of FeC
   martensite
  When FeC martensite with more than
   about 0.2%C are produced by rapid cooling
   from austenite, the reduced interstitial
   spacing of the BCC lattice cause the carbon
   atoms to distort the BCC unit cell along its
   c axis to accommodate the carbon atoms
   (Fig. 9.17c).
  Fig. 9.18 shows how the c axis of the FeC
   martensite lattice is elongated as its carbon
   content increases.
  The hardness and strength of FeC
   martensites are directly related to their
   carbon content and increase as the carbon
   content is increased (Fig.9.19).
  However ductility and toughness also
   decrease with increasing carbon content,
   and so most Martensitic plain-carbon steels
   are tempered by reheating of a temp below
   the transformation temp of 723Co.

10/17/2011                                         6
FIG 9.18
7              10/14/2011
FIG 9.19


8              10/14/2011
Hardness and strength of FeC
     martensite
   Low carbon FeC are strengthened by
    a high concentration of dislocations
    being formed (lath martensite) & by
    interstitial solid solution
    strengthening by carbon atoms.
   The high concentration of
    dislocations in networks (lath
    martensite) makes it difficult for
    other dislocations to move. As the
    carbon content increases above
    0.2%, interstitial solid solution
    strengthening becomes more
    important and the BCC iron lattice
    becomes distorted into tetragonality.
   However, in high carbon FeC
    martensites the numerous twinned
    interfaces in plate martensite also
    contribute to the hardness.

10/17/2011                                  9
   Peritectic reaction At the Peritectic
    reaction point, liquid of 0.53%C combines
    with δ ferrite of 0.09%C to form γ austenite of
    0.17%C. This reaction which occurs at
    1495oC, and can be written as
    Liquid (0.53%C) + δ (0.09%C) 1495oC γ
    (0.17%C)
    γ ferrite is a high-temp phase & so is not
    encountered in plain carbon steels at lower
    temperatures.
   Eutectic reaction At the eutectic
    reaction point, liquid of 4.3% forms γ
    austenite of 2.08%C and the
    intermetallic compound Fe3C, which
    contains 6.67%C. This reaction, which occurs
    at 1148oC, can be written as
   Liquid (4.3%C) 1148oC γ austenite (2.08%C) +
    Fe3C (6.67%C)
    This reaction is not encountered in plain-
    carbon steels because their carbon contents
    are too low.



                                        10/18/2011
                                   10
9.2.3 Invariant reactions in the
     Fe-Fe3C phase diagram
      Eutectoid reaction At the eutectic
       reaction point, solid austenite of 0.8%C
       produces α ferrite with 0.02%C and Fe3C
       that contains 6.67%C. This reaction which
       occurs at 723oC, can be written as
      γ austenite (0.8%C) 723oC α ferrite
       (0.02%C) + Fe3C (6.67%C)
      This eutectic reaction, which takes place
       completely in the solid state, is important
       for some of the heat treatments of plain-
       carbon steels.
      Plain carbon steels that contains 0.8 %C
       is called a eutectoid steel since all-
       eutectoid structure of α ferrite and Fe3C is
       formed when austenite of this composition
       is slowly cooled below the eutectoid
       temperature, If a plain carbon steel
       contains less than 0.8 %C, it is termed a
       hypoeutectoid steel, and if the steel
       contains more than 0.8%C, it is
       designated a hypereutectoid steel.

11                                          10/18/2011
9.2.4 slow cooling of plain
  carbon steels
 Eutectoid plain carbon steels:- If a
  sample of a 0.8%C plain carbon steel is
  heated to about 750oC held for a
  sufficient time, its structure will
  become homogeneous austenite. This
  process is called austsenitizing. If this
  eutectoid steel is then cooled very
  slowly to just above the eutectoid temp,
  its structure will remain austenitic, as
  indicated in Fig. 9.7 at point a.
 Further cooling to the eutectoid temp or
  just below it will cause the entire structure
  to transform from austenite to a lamellar
  structure of alternate plates of α ferrite &
  Cementite. Just below the eutectoid temp,
  at point b in Fig. 9.7, the lamellar structure
  will appear as shown in Fig.9.8. This
  eutectoid structure is called pearlite since it
  resembles mother of pearl. Since the
  solubility of carbon in α ferrite and Fe3C
  changes to very little from 723oC to room
  temp, the pearlite structure will remain
  essentially unchanged in this temp interval.

    10/18/2011                                  12
Fig 9.7
Fig 9.8




10/18/2011   14
Hypoeutectoid plain carbon
       steels
  If a sample of a 0.4%C plain carbon
   steel (Hypoeutectoid steel) is heated
   to about 900oC (point a in Fig.9.9)
   for a sufficient time, its structure will
   become homogeneous austenite.
  Then, if this steel is slowly cooled to
   temp b in Fig.9.9 (about 775oC),
   proeutectoid ferrite will nucleate
   and grow mostly at the austenitic
   grain boundaries.
  If this alloy is slowly cooled from
   temp b to c in Fig.9.9, the amount of
   proeutectoid ferrite formed will
   continue to increase until about 50 %
   of the austenite is transformed.
  While the steel is cooling from b to
   c, the carbon content of the
   remaining austenite will be increased
   from0.4 to 0.8%.

10/18/2011                                     15
10/18/2011
    At 723oC , if very slow cooling
     conditions prevail, the remaining
     austenite will transform
     isothermally into pearlite, the
     eutectoid reaction:
      Austenite → ferrite + cementite.
    The α ferrite in the perlite is
     called eutectoid ferrite to
     distinguish it from the
     proeutectoid ferrite that forms
     first above 723oC.
    Fig.9.10 is an optical micrograph
     of the structure of a 0.35%C
     hypoeutectoid steel that was
     austenitized and slowly cooled to
     room temp.


    10/18/2011                      17
Hypereutectoid plain-carbon
          steels
      If a sample of a 1.2 %C plain carbon steel
         (hypereutectoid steel) is heated to about 950oC
         and held for a sufficient time, its structure will
         become essentially all austenite (point a in
         Fig.9.11).
        Then, if this steel is cooled very slowly to temp b in
         Fig.9.11, proeutectoid cementite will begin to
         nucleate and grow primarily at the austenite grain
         boundaries.
        With further slow cooling to point c of Fig.9.11,
         which is just above 723oC , more proeutectoid
         cementite will be formed at the austenite grain
         boundaries.
        If conditions approaching equilibrium are
         maintained by the slow cooling, the overall carbon
         content of the austenite remaining in the alloy will
         change from 1.2 to 0.8%.
        With still further slow cooling to 723oC or just
         slightly below this temp, the remaining austenite
         will transform to pearlite by the eutectoid reaction,
         as indicated at point d of Fig9.11.
        The cementite formed by the eutectoid reaction is
         called eutectoid cementite to distinguish it from
         the proeutectoid cementite formed at temps above
         723oC.
        Similarly, the ferrite formed by the eutectoid
         reaction is termed eutectoid ferrite. Fig.9.12 is an
19       optical micrograph of the structure of a 1.2%C 10/18/2011
         hypereutectoid steel that was austenitized and
         slowly cooled to room temp.
20
10/14/2011
2
10/14/2011   1
Lath & Plate Martensites




              FIG
              9.13
22                              10/17/2011

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L 07 a

  • 1. L-07 ENGINEERING MATERIALS TRANSFORMATIONS ON HEATING COOLING 10/14/2011 1
  • 2. Microstructure of Fe-C Martensites • Martensite commonly is found in tools such as hammers, chisels and in swords. • Martensite is a hard, brittle form of steel with a tetragonal crystalline structure, created by a process called martensitic transformation. • It is named after metallurgist Adolf Martens (1850-1914), who discovered its structure under his microscope during his metallographic research and explained how the physical properties of different types of steel were affected by their microscopic crystalline structures. 10/17/2011 2
  • 3. Structure of Fe-C on an atomic scale  Martensite is made from austenite, a solid solution of carbon and iron with a face-center cubic crystalline structure that is formed by heating iron to a temperature of at least 723 degrees C.  Martensitic transformation occurs when the austenite is rapidly cooled in a process known as quenching.  The rapid drop in temperature traps carbon atoms inside the crystal structures of the iron atoms before they can diffuse out, resulting in a slight distortion of the shape of these structures that greatly increases the steel's hardness.  The resulting martensitic steel is extremely hard but very brittle. 10/17/2011 3
  • 4. Structure of Fe-C on an atomic scale • Thus, the martensite is then heated in a process called tempering, which causes the martensite to transform partially into ferrite and cementite. This tempered steel sacrifices hardness but results in steel that is tougher and more malleable than pure martensite alone, so it is better suited for industrial use. • For carbon contents in FeC martensites of less than about 0.2%C, the austenite transforms to a BCC ferrite crystal structure. As the carbon content of the FeC alloys is increased, the BCC structure is distorted into a BCT crystal structure. 10/17/2011 4
  • 5. Structure of Fe-C on an atomic scale  The largest interstitial hole in the iron FCC crystal structure has a diameter of 0.104 nm(Fig 9.17a), whereas the largest interstitial hole in the iron BCC structure has a diameter of 0.072 nm (Fig 9.17b). Since the carbon atom has a diameter of 0.154nm, it can be accommodated in interstitial solid solution to a greater extent in the FCC iron lattice. FIG 9.17 5 10/14/2011
  • 6. Hardness and strength of FeC martensite  When FeC martensite with more than about 0.2%C are produced by rapid cooling from austenite, the reduced interstitial spacing of the BCC lattice cause the carbon atoms to distort the BCC unit cell along its c axis to accommodate the carbon atoms (Fig. 9.17c).  Fig. 9.18 shows how the c axis of the FeC martensite lattice is elongated as its carbon content increases.  The hardness and strength of FeC martensites are directly related to their carbon content and increase as the carbon content is increased (Fig.9.19).  However ductility and toughness also decrease with increasing carbon content, and so most Martensitic plain-carbon steels are tempered by reheating of a temp below the transformation temp of 723Co. 10/17/2011 6
  • 7. FIG 9.18 7 10/14/2011
  • 8. FIG 9.19 8 10/14/2011
  • 9. Hardness and strength of FeC martensite  Low carbon FeC are strengthened by a high concentration of dislocations being formed (lath martensite) & by interstitial solid solution strengthening by carbon atoms.  The high concentration of dislocations in networks (lath martensite) makes it difficult for other dislocations to move. As the carbon content increases above 0.2%, interstitial solid solution strengthening becomes more important and the BCC iron lattice becomes distorted into tetragonality.  However, in high carbon FeC martensites the numerous twinned interfaces in plate martensite also contribute to the hardness. 10/17/2011 9
  • 10. Peritectic reaction At the Peritectic reaction point, liquid of 0.53%C combines with δ ferrite of 0.09%C to form γ austenite of 0.17%C. This reaction which occurs at 1495oC, and can be written as Liquid (0.53%C) + δ (0.09%C) 1495oC γ (0.17%C) γ ferrite is a high-temp phase & so is not encountered in plain carbon steels at lower temperatures.  Eutectic reaction At the eutectic reaction point, liquid of 4.3% forms γ austenite of 2.08%C and the intermetallic compound Fe3C, which contains 6.67%C. This reaction, which occurs at 1148oC, can be written as  Liquid (4.3%C) 1148oC γ austenite (2.08%C) + Fe3C (6.67%C) This reaction is not encountered in plain- carbon steels because their carbon contents are too low. 10/18/2011 10
  • 11. 9.2.3 Invariant reactions in the Fe-Fe3C phase diagram  Eutectoid reaction At the eutectic reaction point, solid austenite of 0.8%C produces α ferrite with 0.02%C and Fe3C that contains 6.67%C. This reaction which occurs at 723oC, can be written as  γ austenite (0.8%C) 723oC α ferrite (0.02%C) + Fe3C (6.67%C)  This eutectic reaction, which takes place completely in the solid state, is important for some of the heat treatments of plain- carbon steels.  Plain carbon steels that contains 0.8 %C is called a eutectoid steel since all- eutectoid structure of α ferrite and Fe3C is formed when austenite of this composition is slowly cooled below the eutectoid temperature, If a plain carbon steel contains less than 0.8 %C, it is termed a hypoeutectoid steel, and if the steel contains more than 0.8%C, it is designated a hypereutectoid steel. 11 10/18/2011
  • 12. 9.2.4 slow cooling of plain carbon steels  Eutectoid plain carbon steels:- If a sample of a 0.8%C plain carbon steel is heated to about 750oC held for a sufficient time, its structure will become homogeneous austenite. This process is called austsenitizing. If this eutectoid steel is then cooled very slowly to just above the eutectoid temp, its structure will remain austenitic, as indicated in Fig. 9.7 at point a.  Further cooling to the eutectoid temp or just below it will cause the entire structure to transform from austenite to a lamellar structure of alternate plates of α ferrite & Cementite. Just below the eutectoid temp, at point b in Fig. 9.7, the lamellar structure will appear as shown in Fig.9.8. This eutectoid structure is called pearlite since it resembles mother of pearl. Since the solubility of carbon in α ferrite and Fe3C changes to very little from 723oC to room temp, the pearlite structure will remain essentially unchanged in this temp interval. 10/18/2011 12
  • 15. Hypoeutectoid plain carbon steels  If a sample of a 0.4%C plain carbon steel (Hypoeutectoid steel) is heated to about 900oC (point a in Fig.9.9) for a sufficient time, its structure will become homogeneous austenite.  Then, if this steel is slowly cooled to temp b in Fig.9.9 (about 775oC), proeutectoid ferrite will nucleate and grow mostly at the austenitic grain boundaries.  If this alloy is slowly cooled from temp b to c in Fig.9.9, the amount of proeutectoid ferrite formed will continue to increase until about 50 % of the austenite is transformed.  While the steel is cooling from b to c, the carbon content of the remaining austenite will be increased from0.4 to 0.8%. 10/18/2011 15
  • 17. At 723oC , if very slow cooling conditions prevail, the remaining austenite will transform isothermally into pearlite, the eutectoid reaction: Austenite → ferrite + cementite.  The α ferrite in the perlite is called eutectoid ferrite to distinguish it from the proeutectoid ferrite that forms first above 723oC.  Fig.9.10 is an optical micrograph of the structure of a 0.35%C hypoeutectoid steel that was austenitized and slowly cooled to room temp. 10/18/2011 17
  • 18.
  • 19. Hypereutectoid plain-carbon steels  If a sample of a 1.2 %C plain carbon steel (hypereutectoid steel) is heated to about 950oC and held for a sufficient time, its structure will become essentially all austenite (point a in Fig.9.11).  Then, if this steel is cooled very slowly to temp b in Fig.9.11, proeutectoid cementite will begin to nucleate and grow primarily at the austenite grain boundaries.  With further slow cooling to point c of Fig.9.11, which is just above 723oC , more proeutectoid cementite will be formed at the austenite grain boundaries.  If conditions approaching equilibrium are maintained by the slow cooling, the overall carbon content of the austenite remaining in the alloy will change from 1.2 to 0.8%.  With still further slow cooling to 723oC or just slightly below this temp, the remaining austenite will transform to pearlite by the eutectoid reaction, as indicated at point d of Fig9.11.  The cementite formed by the eutectoid reaction is called eutectoid cementite to distinguish it from the proeutectoid cementite formed at temps above 723oC.  Similarly, the ferrite formed by the eutectoid reaction is termed eutectoid ferrite. Fig.9.12 is an 19 optical micrograph of the structure of a 1.2%C 10/18/2011 hypereutectoid steel that was austenitized and slowly cooled to room temp.
  • 22. Lath & Plate Martensites FIG 9.13 22 10/17/2011