Advanced Structural Steels PDF
Document Details
Tags
Related
- Engineering Materials Past Paper PDF
- ASM Metals Handbook Volume 01 - Properties and Selection of Irons, Steels, and High Performance Alloys PDF
- Module 6: Materials and Hardware PDF
- EVO UT 5.1 PDF - Tecnología de los Materiales (Evaluaciòn) - IC - 2024
- Examen de Tecnología de los Materiales (Evaluaciòn) - IC - 2024 - EVO UT 5.0 - Curso Tarde PDF
- Engineering Alloys PDF
Summary
This document provides an overview of advanced structural steels, focusing on the properties of metals, alloys, and phase transformations. It details the characteristics of different phases and their influence on mechanical properties. It also explores the effects of temperature and composition on the microstructure and properties of steel. Technical details are provided, including diagrams and tables.
Full Transcript
# Advanced Structural Steels ## Metal - Metals are characterized by ductility, malleability, high electrical and thermal conductivity, and high corrosion rate. - Metallic bonding is available in metals, which is responsible for the conductivity of heat and electricity, as there are free electrons w...
# Advanced Structural Steels ## Metal - Metals are characterized by ductility, malleability, high electrical and thermal conductivity, and high corrosion rate. - Metallic bonding is available in metals, which is responsible for the conductivity of heat and electricity, as there are free electrons which enables electron movement required for conductivity. - Metals are divided into 2 categories: - Pure - Alloys ## Alloys - Alloys are materials that consist of at least 2 different atoms, of which at least one of them is metal. - The addition of various elements to a pure metal's lattice structure enables metals to have properties that they do not have in their pure forms. - Generally, alloys are stronger, harder, more durable, and in many cases, more corrosion-resistant compared to their pure metal forms. ## Solid Solution - A homogeneous (one phase structure) mixture of at least two different kinds of atoms in solid state which has a single crystal structure. - Solid Solution ≠ Alloy. - An alloy doesn't have to be consisted of only one phase. - ## Allotropy - If the material has different crystal structures in solid state in accordance with changing temperature and pressure, this is called allotropy. (eg. Fe, Ti) - For most cases it is kept constant at 1 atm. ### Iron Allotropes | Temperature (°C) | Phase | Lattice | a (nm) | Max. C Solubility (%) | |---|---|---|---|---| | 1536 | Liquid | - | - | - | | 1392 | δ-BCC | (ATP: 0.68) | 0.292 | 0.117 | | 912 | γ-FCC | (ATP: 0.74) | 0.355 | 2.06 | | 912 | α-BCC | (ATP: 0.68) | 0.286 | 0.02 | | Room Temperature | - | - | - | 0.008 | ## Main Transition Mechanisms in Fe-C Diagram - **Eutectic:** A liquid transforming into 2 solid phases (T,C constant). - **Peritectic:** One liquid and one solid phase transforming into another solid phase (T,C constant). - **Eutectoid:** One solid phase transforming into 2 different solid phases (T,C constant). ### Fe-C System | Reaction | Products | Temperature (°C) | |---|---|---| | Eutectic | Liquid Fe (4.3%C) → γ (2.06%C) + Fe<sub>3</sub>C (6.67%C) | 1147 | | Peritectic | Liquid Fe (0.52%C) + δ (0.11%) → γ (0.16%) | 1493 | | Eutectoid | γ (0.8%) → α (0.02%) + Fe<sub>3</sub>C (6.67%) | 723 | ## Properties of Fe<sub>3</sub>C (TM: 1320°C) - **Hard** - **Brittle** - **Higher mechanical properties** - Fe<sub>3</sub>C is a transition phase which has properties that are similar to intermetallic phases. - It is considered not only metallic but also covalent and ionic bonding. - Therefore, it has higher mechanical properties. ## Fe-C Diagram - **Acm line:** carbon solubility of Fe is decreasing with decreasing T. - **Led A → γ + Fe<sub>3</sub>C** - **Led γ → pearlite + Fe<sub>3</sub>C** ## Composition 1 (8%C - eutectoid composition) - All carbon content is dissolved in the γ phase, so there is only one phase. - There is a stable γ phase from T₁ to Teutectoid. - At Teutectoid, γ → α + Fe<sub>3</sub>C (all γ phase is transformed to pearlite). #### At Room Temperature - 0.008%C in α - 6.67%C in Fe<sub>3</sub>C ## Applying Lever Rule to obtain phase ratios at room temperature - α% = (6.67-0.8)/(6.67-0.008) * 100 = 88.11% - Fe<sub>3</sub>C% = (0.8-0.008)/(6.67-0.008) * 100 = 11.88% ## Composition 2 (0.3%C) - γ has FCC crystal structure. It can dissolve max. 2.06%C. - a has BCC crystal structure. It can dissolve max. 0.02%C. ## Composition 3 (1.2%C) - solid solution ## Acm Line - Shows that increasing T, increases carbon solubility of γ phase ## TTT diagram - Shows that with increasing cooling rate the microstructure can change. - The microstructure is often called the "steady-state condition" ## Diffusion-Based transformation α → BCC - The volume of the lattice decreases. - This occurs as short range movements of iron atoms. ## Non-equilibrium condition (quenching) - Higher cooling rate in the non-equilibrium condition prevents diffusion based transformation. ## Martensite - A super-saturated structure in terms of carbon is obtained. - As carbon atoms still exist in the lattice, a lattice distortion takes place. - As the result of lattice distortion, the tetragonal structure forms (BCT). - BCT martensite has high strength, high hardness and high brittleness. - Because of the brittle properties BCT martensite can't be directly used an additional heat treatment called tempering should be applied. ## Tempering - Tempering temperature depends on the composition of martensite: - 200-250°C (higher C content only) - 600-650°C (higher C content and also 1 Cr is present) ## Mechanical properties of martensite - **Composition:** If we have lower C content than 0.22%C, we can't obtain martensite as we can't have a super-saturated structure. - **Microstructure:** - Lath martensite: higher strength and hardness than plate martensite. - Plate martensite: higher proportion and higher ductility than lath martensite. ## Martensite Microstructure - **Grain size:** With exception of creep, finer grain size results in improvement of mechanical properties. - **Initial Microstructure:** Initially the microstructure of & directly affects the microstructure of martensite. With increased temperature, the grain sizes also increase. So, cooling that is approx. 30-50°C above A₁ line is favorable from a temperature met is approx. 30-50°C above A₁ line is favorable. - **Martensite doesn't appear in the Fe- Fe<sub>3</sub>C phase diagram as the phase diagram is drawn for equilibrium condition.** - TTT (Time-Temperature-Transformation) diagram should be examined in order to investigate martensite. ## Cooling Rates - After cooling α down by 3 different cooling rates (1, 3, 4), a similar martensite, super saturated carbon structure and lattice distortion can be achieved. - However, as high cooling rate contributes to high internal stress, a higher cooling rate is preferred to obtain martensite.