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Growth of Solid Equilibrium - Science and Engineering of Materials - Lecture Slides, Slides of Materials science

These are the Lecture Slides of Science and Engineering of Materials which includes Point Defects, Types of Defects, Equilibrium Number, Thermal Vibrations, Boltzmann Constant, Regular Lattice Sites, Substitutional Solid Solutions, Composition Conversions etc. Key important points are: Growth of Solid Equilibrium, Non-Equilibrium Cooling, Solid Solution Strengthening, Isomorphous Alloys, Binary Eutectic Systems, Eutectic Reaction, Microstructure in Eutectic Alloys, Eutectic Isotherm

Typology: Slides

2012/2013

Uploaded on 03/21/2013

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Growth of Solid
Equilibrium ( = very slow cooling)
In solid + liquid phase region: Solid forms
gradually upon cooling from liquidus line
Composition of solid and liquid changes
gradually (determine by tie-line method)
At the solidus line: solid nuclei grow to
consume all the liquid
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Growth of Solid Equilibrium ( = very slow cooling)

In solid + liquid phase region: Solid forms gradually upon cooling from liquidus line

Composition of solid and liquid changes gradually (determine by tie-line method)

At the solidus line: solid nuclei grow to consume all the liquid

Microstructure in isomorphous alloys Non-equilibrium cooling

  • Compositional change requires diffusion
  • Liquid: diffusion if fast (tie-line OK)
  • Solid state: diffusion is SLOW

(no tie line) ⇒ New layers solidifying on grains have the equilibrium composition at that T ⇒ Formation of layered (cored) grains

  • On heating: grain boundaries melt first. Can lead to premature mechanical failure.

Average Ni content of grains is higher?

Application of the lever rule

Greater proportion of liquid phase as compared to equilibrium at the same T

Solidus line is shifted to the righthigher Ni content

Solidification complete at lower TOuter part of grains are richer in the low-melting component (Cu).

Mechanical properties of isomorphous alloys

Solid solution strengthening

Three single phase regions α - solid solution Ag in Cu matrix, β = solid solution of Cu in Ag matrix, L - liquid

Three two-phase regions (α + L, β +L, α +β)

Solvus separates one solid solution from a mixture of solid solutions. Solvus ⇒ limit of solubility

Copper – Silver phase diagram

Binary Eutectic System

Binary Eutectic System

Eutectic (invariant) point Liquid + two solid phases co-exist Eutectic composition C (^) E Eutectic temperature TE. Eutectic Isotherm - horizontal solidus line at TE

Lead – Tin phase diagram

Invariant or eutectic point

Eutectic isotherm

Binary Eutectic System

Compositions + relative amounts of phases ⇒ Tie line and lever rule

  • C
  • B
  • A

Microstructure in eutectic alloys

Cooling of liquid lead/tin system at different compositions

Lead-rich alloy (0-2 wt% tin)

Solidification proceeds as for isomorphous alloys

L → α +L → α

No changes above eutectic temperature, T (^) E At T (^) E liquid transforms to α and β phases (eutectic reaction)

L → α + β

Solidification at Eutectic composition

Solidification at Eutectic composition

α and β compositions are very different ⇒ Eutectic reaction ⇒ redistribution of Pb and Sn atoms by diffusion Simultaneous formation of α and β phases ⇒ layered (lamellar) microstructure: eutectic structure

Formation of eutectic structure in lead-tin system. Dark layers are lead-rich α phase. Light layers are the tin-rich β phase.

Microstructure in eutectic alloys Microconstituent – element of microstructure having a distinctive structure. For previous page: microstructure ⇒ two microconstituents: primary α and eutectic structure.

Although the eutectic structure consists of two phases, it is a microconstituent with distinct lamellar structure and fixed ratio of the two phases.

Relative amounts of microconstituents

Treat eutectic as separate phase + apply lever rule

Fractions: primary α phase (18.3 wt% Sn) and eutectic structure (61.9 wt% Sn):

We = P / (P+Q) ; Wα’ = Q / (P+Q)