10/8/2009 Prof. A.K.M.B. Rashid Department of MME BUET, Dhaka Concept of alloying Classification of alloys Introduction to the phase diagram Uses and limitations of phase diagrams Classification of phase diagrams Construction of phase diagrams Reference: 1. Avner. Introduction to Physical Metallurgy, Ch. 5 and 6. © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 02 1 10/8/2009 An alloy is a substance that has metallic properties and is composed of two or more chemical elements, of which at least one is a metal. Alloying elements are deliberately introduced into a metal to enhance properties (especially, mechanical properties) 60% Ni Monel Note the difference z Alloy and alloy system z Alloying element and impurity element Alloy systems z Binary system (Fe-C system, Cu-Zn system) z Ternary system (Fe-C-Mn system, Al-Si-Mg system) © Rashid, DMME, BUET . 2009 Cu Wt % Nickel Property Ni Direction Tensile strength Yield Strength % Elongation Electrical Conductivity MME 291, Lec 03: Introduction to phase diagrams Up Up Down Down P 03 Classifications based on: X Structure (e.g., austenitic stainless steel) yp of p phase diagram g ((e.g., g , eutectic alloys) y ) Y Type Alloy can be homogeneous or mixture. In the solid state, there are three possible phases exist: X Pure metal y phase p or compound p Y Intermediate alloy Z Solid solution If the alloy is a mixture, then any combination of the above three phases is possible in the solid state. © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 04 2 10/8/2009 Intermediate Alloy Phases, or Compounds Intermediate chemical composition; different crystal structure Expressed by chemical formula Congruently melting, exhibiting definite melting point (like metals) X Intermetallic compounds (Mg2Pb, Mg2Sn, ....) Ñ Ñ Ñ Ñ formed between chemically dissimilar metals have strong ionic/covalent bond nonmetallic properties (poor ductility, poor conductivity) complex strucutre Y Interstitial compounds (Fe3C, Fe4N, TiC, .....) Ñ formed between transition metals and H/O/C/N/B Ñ small atoms of nonmetals go into the interstitices of metals Ñ metallic properties, narrow composition range, extremely hard, high melting point Z Electron compounds (AgZn, FeAl, Cu3Si, ....) Ñ form structure similar to constituting elements Ñ have a definite ratio of valence electrons Ñ properties similar to solid solutions (wide composition range, high ductility, low hardness Solid Solutions Solution in the solid state where two kinds of atoms are combined bi d in i one crystall lattice. l i Distortion resulted during formation of solution causes an increase in strength of the alloy. This is the primary basis for strengthening of a metal by alloying. Solubility of solute in solution depends on temperature and pressure of the system, and method of forming. Unsaturated, saturated, and supersaturated solutions © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 06 3 10/8/2009 Solid Solutions Substitutional and interstitial solid solutions Interstitial Substitutional Hume Rothery Rule for forming Hume-Rothery substitutional solid solution X Y Z [ Crystal structure factor Relative size factor Chemical affinity factor Relative valence factor © Rashid, DMME, BUET . 2009 Example: Cu – Ni alloy ⇒ Completely soluble Cu – Zn alloy ⇒ Partially soluble Cu – Pb alloy ⇒ Completely insoluble MME 291, Lec 03: Introduction to phase diagrams P 07 Summary of Possible Alloy Structures © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 08 4 10/8/2009 z We have seen how the structure of materials control their properties. z So it is important that we must know X about the structure of a material that has been developed during its manufacture, and Y the method of controlling (and/or modifying) the structure to enhance its properties. z Phase diagram is an important tool for materials scientists that tells which phases are stable in a system under specified conditions (e.g. of temperature, overall composition, pressure) © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams z Phase diagram is basically a map that presents the domains of stability of phases and the limits of stability of phases in a graphical form. z Reading the map will tell you, at the state when it comes to equilibrium, P 09 liquid solid gas liquid-gas equilibria Temperature Typical phase diagram for one component system 1. what phases are present, 2. the state of those phases, and 3 the relative quantities of each phase 3. phase. z Reading a phase diagram will also tell what phase transformations we can expect when we change one of the parameters of the system (T, P, X). © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 10 5 10/8/2009 Components Chemically recognisable species that are mixed to f form the h alloy. ll z In Brass: Cu, Zn (element) z In steels: Fe, C (element) z In ceramics: SiO2, Al2O3 (compound) Binary alloy contains 2 components, ternary 3, etc. Phase A phase is a homogenous, physically distinct and mechanically separable portion of the material with a given chemical composition and structure. © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 11 What and how many phases materials possess? z Solid, liquid, or gas, (and plasma)? z Is it possible to have more than one solid phases? Iron, being an allotropic material, has more than one solid phases: When iron first freezes from its liquid state, it is BCC (δ-iron) As it cools it changes to FCC (γ-iron) Upon further cooling it changes to BCC (α-iron) © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 12 6 10/8/2009 Microstructure Microstructure of Al-Cu Alloy z The properties of an alloy depend not only on proportions of the phases but also on how they are arranged structurally at the microscopic level. z Thus, the microstructure is specified by the number of phases, their proportions, and their arrangement in space. space α phase (darker) Microstructure of Cast Iron z Phase diagrams will help us to understand and predict the microstructures like the one shown in this page © Rashid, DMME, BUET . 2009 β phase ((lighter) g ) MME 291, Lec 03: Introduction to phase diagrams pearlite (finger print) graphite (grey) P 13 Equilibrium state and Metastable state A system is at equilibrium if at constant T pressure andd composition T, iti the th system t is i stable, not changing with time. The equilibrium state always has the minimum free energy. z Equilibrium state requires sufficient time to achieve. When this time is too longg ((due to slow kinetics), another state along the path to the equilibrium may appear to be stable. This is called a metastable state. z A system at a metastable state is trapped in a local minimum of free energy, which is not the global one. © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 14 7 10/8/2009 z Selection of alloys showing enhanced characteristics in: 5 5 5 5 Brazing B i and d soldering ld i Diffusion problems Corrosion Electrical resistivity z Manipulation of phase transformations of materials to control their properties Phase diagrams are also known as the equilibrium diagrams. Rate of phase transformations is missing. TTT (Temperature-Time-Transformation) diagrams are a complement to phase diagrams. © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 15 One component (unary) phase diagrams Also known as P T diagrams. P-T di The simple case is Water. z z z How many single-phase regions? How many two-phase regions? Is there any three-, or more-phase regions? Gibb’s Phase Rule: F = C–P+2 F = # variables C = # components P = # phases © Rashid, DMME, BUET . 2009 Unary phase diagram of water MME 291, Lec 03: Introduction to phase diagrams P 16 8 10/8/2009 Binary (two-component) phase diagrams How does mixing of A into B effect the bond energies andd the th melting lti temperature t t off the th resultant lt t alloy? ll ? Interaction of A and B resulted three bonds: A-A, B-B and A-B bonds. In ideal cases: (A-B) = x (A-A) + (1-x) (B-B) TAlloy = TA + x (TB – TA) where x is mole fraction of A in B Must follow Hume Rothery Rule Example: Copper - Nickel, Silicon - Germanium Î Completely miscible/soluble phase diagrams © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 17 Binary (two-component) phase diagrams Ni-Cu phase diagram (completely miscible) 9 10/8/2009 Binary (two-component) phase diagrams Ge-Si phase diagram (completely miscible) Binary (two-component) phase diagrams When A-B < 0.5 (A-A + B-B) then TAlloy < TA , TB Example: Lead - Tin, Tin Gold - Silicon, Silicon Copper - Silver Î Eutectic phase diagrams X Completely immiscible/insoluble phase diagrams Y Partially miscible/soluble phase diagrams © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 20 10 10/8/2009 Binary (two-component) phase diagrams Au-Si phase diagram (Completely insoluble) Binary (two-component) phase diagrams Cu-Ag phase diagram (Partially soluble) 11 10/8/2009 Binary (two-component) phase diagrams Pb-Sn phase diagram (Partially soluble) Binary (two-component) phase diagrams Au-Ge phase diagram (Partially soluble) 12 10/8/2009 Binary (two-component) phase diagrams When A-B > 0.5 (A-A + B-B) then TAlloy > TA , TB Example: E l G lli Gallium - Arsenic, A i Aluminium Al i i - Antimony A ti Î Intermetallic compound formation © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 25 Binary (two-component) phase diagrams Al-Sb phase diagram 13 10/8/2009 Theoretical Construction z By applying thermodynamic principles z Use of software like Thermocalc Experimental Methods X Thermal analysis z Generation of cooling curves (temperature vs. time) for a number of alloys of the alloy system to obtain arrest points (temperatures where a change in slope is observed) z Solid-state phase changes are difficult to obtained in this method Y Metallographic M ll hi method h d z Heating samples of an alloy to different temperatures, and quench them after equilibrium to retain the high-temperature structure z Observe the structure microscopically z Rapidly cooled samples do not always retain high-temperature structures; considerable skill is required to interpret the microstructure correctly © Rashid, DMME, BUET . 2009 MME 291, Lec 03: Introduction to phase diagrams P 27 14
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