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The document discusses the microstructure and properties of martensite steel. It contains the following key points: 1) Martensite is a hard, brittle form of steel created by rapid cooling of austenite steel. It has a tetragonal crystal structure. 2) During rapid cooling, carbon atoms are trapped in the iron crystal structure, distorting it and increasing hardness. 3) Martensite steel is made harder but brittle. Tempering involves reheating to partially transform martensite into ferrite and cementite, increasing toughness at the cost of hardness.
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- 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
- 13. Fig 9.7
- 14. Fig 9.8 10/18/2011 14
- 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
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- 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
- 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.
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- 22. Lath & Plate Martensites FIG 9.13 22 10/17/2011